CN111123487B

CN111123487B - Infrared lens

Info

Publication number: CN111123487B
Application number: CN201911380240.8A
Authority: CN
Inventors: 孙加安; 王�锋; 周明明; 马庆鸿; 万良伟
Original assignee: Huizhou Xingjuyu Optical Co ltd
Current assignee: Guangdong Xingjuyu Optical Co ltd
Priority date: 2019-12-27
Filing date: 2019-12-27
Publication date: 2021-12-21
Anticipated expiration: 2039-12-27
Also published as: CN111123487A

Abstract

The invention provides an infrared lens, which sequentially comprises the following components from an object side to an image side: a first lens, a second lens, a third lens and a fourth lens; the surface of the object side of the first lens is a convex surface, the surface of the image side of the first lens is a concave surface, and the first lens has positive focal power; the surface of the object side of the second lens is a convex surface, the surface of the image side of the second lens is a concave surface, and the second lens has positive focal power; the object side surface of the third lens is a convex surface; the focal length of the infrared lens is f, the focal length of the first lens is f1, and the following relation is satisfied: 3.00< f1/f < 4.84. The invention has the beneficial effects that: the infrared imaging and depth perception are realized under the condition of ensuring compact structure, and the advantages of better imaging quality, lower production cost and the like are achieved; by using the lens made of the visible light filtering material, most visible light can be filtered by the lens, so that infrared imaging is clearer, and less visible light interference is caused.

Description

Infrared lens

[ technical field ] A method for producing a semiconductor device

The invention relates to the technical field of optical lenses, in particular to an infrared lens.

[ background of the invention ]

In recent years, with the rise of smart phones, the demand of miniaturized camera lenses is gradually increasing, and the photosensitive devices of general camera lenses are not limited to two types, namely, a Charge Coupled Device (CCD) or a Complementary Metal-oxide semiconductor (CMOS) Sensor, and due to the refinement of semiconductor manufacturing technology, the pixel size of the photosensitive devices is reduced, and in addition, the current electronic products are developed in a form of being excellent in function, light, thin, short and small, so that the miniaturized infrared lens with good imaging quality is the mainstream in the current market.

In the related art, in order to obtain better imaging quality, a multi-piece lens structure is mostly adopted in a lens traditionally mounted on a mobile phone camera, a television, a motion sensing game machine and the like, but with the increase of lenses, the lens is heavy in volume, the production cost is increased, the imaging quality is reduced, and long-focus shooting is difficult to realize.

[ summary of the invention ]

Based on this, it is necessary to design an infrared lens, which can realize telephoto shooting under the condition of ensuring compact structure, and has the advantages of better imaging quality, lower production cost, clearer infrared imaging, less interference by visible light, and the like.

In order to achieve the purpose, the technical scheme provided by the invention is as follows:

an infrared lens, comprising, in order from an object side to an image side: a first lens, a second lens, a third lens and a fourth lens;

the surface of the object side of the first lens is a convex surface, the surface of the image side of the first lens is a concave surface, and the first lens has positive focal power; the surface of the object side of the second lens is a convex surface, the surface of the image side of the second lens is a concave surface, and the second lens has positive focal power; the object side surface of the third lens is a convex surface;

the focal length of the infrared lens is f, the focal length of the first lens is f1, and the following relation is satisfied:

3.00<f1/f<4.84。

preferably, the radius of curvature of the object-side surface of the second lens is R21, the radius of curvature of the image-side surface of the second lens is R22, and the following relationship is satisfied:

0.47＜R21/R22＜0.88。

preferably, the focal length of the infrared lens is f, the focal length of the second lens is f2, and the following relation is satisfied:

2.00<f2/f<7.96。

preferably, the air space between the first lens and the second lens on the optical axis is AG12, the center thickness of the second lens on the optical axis is CT2, and the following relation is satisfied:

0.43<AG12/CT2<1.01。

preferably, the total optical length of the infrared lens is TTL, and the half-image height of the infrared lens is ImgH, and satisfies the following relation:

1.71<TTL/ImgH<1.75。

preferably, the total optical length of the infrared lens is TTL, and the back focal length of the infrared lens is BFL, and satisfies the following relation:

5.29<TTL/BFL<6.24。

the present invention further provides an infrared lens, which, in order from an object side to an image side, comprises: a first lens, a second lens, a third lens and a fourth lens;

the central thickness of the first lens on the optical axis is CT1, the sum of the central thicknesses of the first lens to the fourth lens on the optical axis is Sigma CT, and the following relations are satisfied:

0.13<CT1/ΣCT<0.21。

the invention has the beneficial effects that:

1. the infrared imaging and depth perception are realized under the condition of ensuring compact structure, and the advantages of better imaging quality, lower production cost and the like are achieved;

2. by using the lens made of the visible light filtering material, most visible light can be filtered by the lens, so that infrared imaging is clearer, and less visible light interference is caused.

[ description of the drawings ]

In order to more clearly illustrate the technical solutions of the embodiments of the present invention, the drawings needed to be used in the embodiments will be briefly described below, it should be understood that the following drawings only illustrate some embodiments of the present invention and therefore should not be considered as limiting the scope, and for those skilled in the art, other related drawings can be obtained according to the drawings without inventive efforts.

Fig. 1 is a schematic structural diagram of an infrared lens according to embodiment 1 of the present invention;

fig. 2 is a spherical aberration graph of the infrared lens of embodiment 1;

fig. 3 is a graph showing astigmatism and distortion of the infrared lens of example 1;

fig. 4 is a graph of chromatic aberration of magnification of the infrared lens of embodiment 1;

fig. 5 is a schematic structural view of an infrared lens according to embodiment 2 of the present invention;

fig. 6 is a spherical aberration graph of the infrared lens of embodiment 2;

fig. 7 is a graph showing astigmatism and distortion of the infrared lens of example 2;

fig. 8 is a graph of chromatic aberration of magnification of the infrared lens of embodiment 2;

fig. 9 is a schematic structural view of an infrared lens according to embodiment 3 of the present invention;

fig. 10 is a spherical aberration graph of the infrared lens of embodiment 3;

fig. 11 is a graph of astigmatism and distortion of the infrared lens of embodiment 3;

fig. 12 is a graph of chromatic aberration of magnification of the infrared lens of embodiment 3;

fig. 13 is a schematic structural view of an infrared lens according to embodiment 4 of the present invention;

fig. 14 is a spherical aberration chart of the infrared lens of embodiment 4;

fig. 15 is a graph showing astigmatism and distortion of the infrared lens of example 4;

fig. 16 is a graph of chromatic aberration of magnification of the infrared lens of embodiment 4;

fig. 17 is a schematic structural view of an infrared lens according to embodiment 5 of the present invention;

fig. 18 is a spherical aberration chart of the infrared lens of embodiment 5;

fig. 19 is a graph showing astigmatism and distortion of the infrared lens of example 5;

fig. 20 is a graph of chromatic aberration of magnification of the infrared lens of embodiment 5;

fig. 21 is a schematic structural view of an infrared lens according to embodiment 6 of the present invention;

fig. 22 is a spherical aberration graph of the infrared lens of embodiment 6;

fig. 23 is a graph showing astigmatism and distortion of the infrared lens of example 6;

fig. 24 is a chromatic aberration of magnification graph of an infrared lens of embodiment 6;

fig. 25 is a schematic structural view of an infrared lens according to embodiment 7 of the present invention;

fig. 26 is a spherical aberration chart of the infrared lens of embodiment 7;

fig. 27 is a graph of astigmatism and distortion of the infrared lens of example 7;

fig. 28 is a chromatic aberration of magnification graph of the infrared lens of embodiment 7.

[ detailed description ] embodiments

To facilitate an understanding of the invention, the invention will now be described more fully with reference to the accompanying drawings. Preferred embodiments of the present invention are shown in the drawings. This invention may, however, be embodied in many different forms and should not be construed as limited to the embodiments set forth herein. Rather, these embodiments are provided so that this disclosure will be thorough and complete.

It will be understood that when an element is referred to as being "secured to" another element, it can be directly on the other element or intervening elements may also be present. When an element is referred to as being "connected" to another element, it can be directly connected to the other element or intervening elements may also be present. The terms "vertical," "horizontal," "left," "right," and the like as used herein are for illustrative purposes only and do not represent the only embodiments.

Unless defined otherwise, all technical and scientific terms used herein have the same meaning as commonly understood by one of ordinary skill in the art to which this invention belongs. The terminology used herein in the description of the invention is for the purpose of describing particular embodiments only and is not intended to be limiting of the invention. As used herein, the term "and/or" includes any and all combinations of one or more of the associated listed items.

Referring to fig. 1, the present invention provides an infrared lens including four lenses, specifically, the infrared lens 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, and a fourth lens L4.

The infrared lens of the present invention may include an optical imaging system composed of four lenses. That is, the infrared lens may be configured by the first lens L1 to the fourth lens L4. However, the infrared lens is not limited to including four lenses, but may include other constituent elements as needed. For example, the infrared lens further includes an aperture that adjusts the amount of light. In addition, an optical filter and an image plane may be sequentially disposed on the image side surface close to the fourth lens, an image sensor is disposed on the image plane, the image sensor may be any of various image sensors in the prior art, that is, the image sensor converts the light image on the light sensing surface into an electrical signal in a proportional relationship with the light image by using a photoelectric conversion function of a photoelectric device, and the image sensor is a functional device that divides the light image on the light receiving surface into a plurality of small cells and converts the small cells into usable electrical signals, compared with a photosensitive element of a "point" light source such as a photodiode and a phototriode.

Therefore, light rays refracted by external things sequentially pass through the first lens to the fourth lens, then enter the image plane through the optical filter, and are converted into conductive electric signals through the image sensor on the image plane.

Further, the first lens L1, the second lens L2, the third lens L3, and the fourth lens L4 are plastic lenses or glass lenses. The first lens L1 to the fourth lens L4 are four independent lenses, and a space is provided between every two adjacent lenses, that is, every two adjacent lenses are not joined to each other, but an air space is provided between every two adjacent lenses. Since the process of joining the lenses is more complicated than that of the independent and non-joined lenses, particularly, the joining surfaces of the two lenses need to have a curved surface with high accuracy so as to achieve high joint tightness when the two lenses are joined, and poor adhesion tightness due to deviation may be caused during the joining process to affect the overall optical imaging quality.

Referring to fig. 1, the object-side surface of the first lens element L1 is convex, the image-side surface of the first lens element L1 is concave, and the first lens element L1 has positive refractive power; the object-side surface of the second lens element L2 is convex, the image-side surface of the second lens element L2 is concave, and the second lens element L2 has positive refractive power; the object-side surface of the third lens L3 is convex. The focal length of the infrared lens is f, the focal length of the first lens is f1, and the following relation is satisfied: 3.00< f1/f < 4.84.

In another embodiment of the present invention, the central thickness of the first lens on the optical axis is CT1, the sum of the central thicknesses of the first to fourth lenses on the optical axis is Σ CT, and the following relation is satisfied: 0.13< CT1/Σ CT < 0.21.

More specifically, the infrared lens includes, in order from the object side to the image side along the optical axis, four lenses L1-L4, a first lens L1 having an object side surface S1 and an image side surface S2; the second lens L2 has an object-side surface S3 and an image-side surface S4; the third lens L3 has an object-side surface S5 and an image-side surface S6; the fourth lens L4 has an object-side surface S7 and an image-side surface S8. Optionally, the infrared lens may further include a filter L5 having an object side S9 and an image side S10, and the filter L5 may be a band pass filter. In the image pickup optical lens group of the present embodiment, a stop STO may also be provided to adjust the amount of light entering. The light from the object sequentially passes through the respective surfaces S1 to S8 and is finally imaged on the imaging surface S11.

Further, the total optical length of the infrared lens is TTL, and the half-image height of the infrared lens is ImgH, and satisfies the following relation: 1.71< TTL/ImgH < 1.75.

Further, the radius of curvature of the object-side surface of the second lens is R21, the radius of curvature of the image-side surface of the second lens is R22, and the following relation is satisfied: 0.47 < R21/R22 < 0.88.

Further, the focal length of the infrared lens is f, the focal length of the second lens is f2, and the following relation is satisfied: 2.00< f2/f < 7.96.

Further, the air interval of the first lens and the second lens on the optical axis is AG12, the center thickness of the second lens on the optical axis is CT2, and the following relation is satisfied: 0.43< AG12/CT2< 1.01.

Further, the total optical length of the infrared lens is TTL, and the back focal length of the infrared lens is BFL, and satisfies the following relation: 5.29< TTL/BFL < 6.24.

The infrared lens according to the above-described embodiment of the present invention may employ a plurality of lenses, for example, four lenses as described above. Through reasonable distribution of focal power, surface type and on-axis distance of each lens, the effective light passing diameter of the infrared lens can be effectively increased, miniaturization of the lens is guaranteed, imaging quality is improved, and the infrared lens is more favorable for production and processing. In the embodiment of the present invention, at least one of the mirror surfaces of each lens is an aspherical mirror surface. The aspheric lens is characterized in that: the curvature varies continuously from the center to the periphery of the lens. Unlike a spherical lens having a constant curvature from the center to the periphery of the lens, an aspherical lens has a better curvature radius characteristic, has the advantages of improving distortion aberration and astigmatic aberration, and can make the field of view larger and more realistic. After the aspheric lens is adopted, the aberration generated in imaging can be eliminated as much as possible, so that the imaging quality is improved.

Specific examples of the infrared lens that can be applied to the above-described embodiments are further described below with reference to the drawings.

Example 1

An infrared lens according to embodiment 1 of the present invention is described below with reference to fig. 1 to 4. Fig. 1 shows a schematic structural diagram of an infrared lens according to embodiment 1 of the present invention.

As shown in fig. 1, the infrared lens includes, in order from an object side to an image side, four lenses L1-L4, a first lens L1 having an object side surface S1 and an image side surface S2; the second lens L2 has an object-side surface S3 and an image-side surface S4; the third lens L3 has an object-side surface S5 and an image-side surface S6; the fourth lens L4 has an object-side surface S7 and an image-side surface S8. Optionally, the infrared lens may further include a filter L5 having an object side S9 and an image side S10, and the filter L5 may be a band pass filter. In the infrared lens of the present embodiment, a stop STO may also be provided to adjust the amount of incoming light. The light from the object sequentially passes through the respective surfaces S1 to S10 and is finally imaged on the imaging surface S11.

The effective focal length EFL, the full field angle FOV, the total optical length TTL, the aperture Fno, the surface type, the curvature radius, the thickness, the material and the conic coefficient of the infrared lens in embodiment 1 are shown in table 1:

TABLE 1

As can be seen from table 1, OBJ denotes a light source; the focal length of the infrared lens is f, the focal length of the first lens is f1, and the following relation is satisfied: 3.00< f1/f <4.84, specifically, f1/f 3.955; the total optical length of the infrared lens is TTL, the half-image height of the infrared lens is imgH, and the following relational expression is satisfied: 1.71< TTL/ImgH <1.75, specifically, 1.732; the optical total length of the infrared lens is TTL, the back focal length of the infrared lens is BFL, and the following relational expression is satisfied: 5.29< TTL/BFL <6.24, specifically, TTL/BFL ═ 5.777; the focal length of the infrared lens is f, the focal length of the second lens is f2, and the following relation is satisfied: 2.00< f2/f <7.96, specifically, f2/f is 2.247.

In the embodiment, four lenses are taken as an example, and the focal power and the surface type of each lens are reasonably distributed, so that the aperture of the lens is effectively enlarged, the total length of the lens is shortened, and the effective light transmission diameter of the lens and the miniaturization of the lens are ensured; meanwhile, various aberrations are corrected, and the resolution and the imaging quality of the lens are improved. Each aspheric surface type x is defined by the following functional relationship:

the aspheric function relationship of the infrared lens is as follows:

wherein x is the rise of the distance from the aspheric surface vertex to the aspheric surface vertex when the aspheric surface is at the position with the height of h along the optical axis direction; c is the paraxial curvature of the aspheric surface, c being 1/r (i.e., paraxial curvature c is the inverse of radius of curvature r in table 2 above); k is the conic constant (given in table 1 above); ai is a correction coefficient of the i-n th order of the aspherical surface, and the coefficients of the high-order terms A4, A6, A8, A10, A12, A14 and A16 of the respective lens surfaces S1-S8 are shown in Table 2:

TABLE 2

As can be seen from tables 1 and 2, in this embodiment, the central thickness of the first lens on the optical axis is CT1, the sum of the central thicknesses of the first to fourth lenses on the optical axis is Σ CT, and the following relationship is satisfied: 0.13< CT1/Σ CT <0.21, specifically, CT1/Σ CT is 0.169; the curvature radius of the object side surface of the second lens is R21, the curvature radius of the image side surface of the second lens is R22, and the following relations are satisfied: 0.47 < R21/R22 < 0.88, specifically, R21/R22 is 0.511. The air space between the first lens and the second lens on the optical axis is AG12, the central thickness of the second lens on the optical axis is CT2, and the following relations are satisfied: 0.43< AG12/CT2<1.01, specifically, AG12/CT2 is 0.644.

Fig. 2 shows a spherical aberration curve of the infrared lens of embodiment 1, which shows that light rays of different aperture angles U intersect the optical axis at different points, and have different deviations from the position of an ideal image point. Fig. 3 shows astigmatism curves of the infrared lens of embodiment 1, which represent meridional field curvature and sagittal field curvature. Fig. 3 shows distortion curves of the infrared lens of embodiment 1, which represent distortion magnitude values in the case of different viewing angles. Fig. 4 shows a chromatic aberration of magnification curve of the infrared lens of embodiment 1, which represents a deviation of different image heights on an image plane after light passes through the infrared lens. As can be seen from fig. 2 to 4, the infrared lens according to embodiment 1 can achieve good imaging quality.

Example 2

An infrared lens according to embodiment 2 of the present invention is described below with reference to fig. 5 to 8. Fig. 5 is a schematic structural diagram illustrating an infrared lens according to embodiment 2 of the present invention.

As shown in fig. 5, the infrared lens includes, in order from an object side to an image side, four lenses L1-L4, a first lens L1 having an object side surface S1 and an image side surface S2; the second lens L2 has an object-side surface S3 and an image-side surface S4; the third lens L3 has an object-side surface S5 and an image-side surface S6; the fourth lens L4 has an object-side surface S7 and an image-side surface S8. Optionally, the infrared lens may further include a filter L5 having an object side S9 and an image side S10, and the filter L5 may be a band pass filter. In the infrared lens of the present embodiment, a stop STO may also be provided to adjust the amount of incoming light. The light from the object sequentially passes through the respective surfaces S1 to S10 and is finally imaged on the imaging surface S11.

The effective focal length EFL, the full field angle FOV, the total optical length TTL, the aperture Fno, the surface type, the curvature radius, the thickness, the material and the conic coefficient of the infrared lens in embodiment 2 are shown in table 3:

TABLE 3

As can be seen from table 3, OBJ denotes a light source; the focal length of the infrared lens is f, the focal length of the first lens is f1, and the following relation is satisfied: 3.00< f1/f <4.84, specifically, f1/f — 3.757; the total optical length of the infrared lens is TTL, the half-image height of the infrared lens is imgH, and the following relational expression is satisfied: 1.71< TTL/ImgH <1.75, specifically, TTL/ImgH is 1.730; the optical total length of the infrared lens is TTL, the back focal length of the infrared lens is BFL, and the following relational expression is satisfied: 5.29< TTL/BFL <6.24, specifically, TTL/BFL ═ 5.764; the focal length of the infrared lens is f, the focal length of the second lens is f2, and the following relation is satisfied: 2.00< f2/f <7.96, specifically, f2/f is 2.001.

the aspheric function relationship of the infrared lens is as follows:

wherein x is the rise of the distance from the aspheric surface vertex to the aspheric surface vertex when the aspheric surface is at the position with the height of h along the optical axis direction; c is the paraxial curvature of the aspheric surface, c being 1/r (i.e., paraxial curvature c is the inverse of radius of curvature r in table 2 above); k is the conic constant (given in table 3 above); ai is a correction coefficient of the i-n th order of the aspherical surface, and the coefficients of the high-order terms a4, a6, A8, a10, a12, a14, and a16 of the respective lens surfaces S1 through S8 are shown in table 4:

TABLE 4

As can be seen from tables 3 and 4, in this embodiment, the central thickness of the first lens on the optical axis is CT1, the sum of the central thicknesses of the first to fourth lenses on the optical axis is Σ CT, and the following relationship is satisfied: 0.13< CT1/Σ CT <0.21, specifically, CT1/Σ CT is 0.165; the curvature radius of the object side surface of the second lens is R21, the curvature radius of the image side surface of the second lens is R22, and the following relations are satisfied: 0.47 < R21/R22 < 0.88, specifically, R21/R22 is 0.471; the air space between the first lens and the second lens on the optical axis is AG12, the central thickness of the second lens on the optical axis is CT2, and the following relations are satisfied: 0.43< AG12/CT2<1.01, specifically, AG12/CT2 is 0.685.

Fig. 6 shows a spherical aberration curve of the infrared lens of embodiment 2, which shows that light rays of different aperture angles U intersect the optical axis at different points, and have different deviations from the position of an ideal image point. Fig. 7 shows astigmatism curves of the infrared lens of embodiment 2, which represent meridional field curvature and sagittal field curvature. Fig. 7 shows distortion curves of the infrared lens of embodiment 2, which represent distortion magnitude values in the case of different viewing angles. Fig. 8 shows a chromatic aberration of magnification curve of the infrared lens of embodiment 2, which represents a deviation of different image heights on an image plane after light passes through the infrared lens. As can be seen from fig. 6 to 8, the infrared lens according to embodiment 2 can achieve good imaging quality.

Example 3

An infrared lens according to embodiment 3 of the present invention is described below with reference to fig. 9 to 12. Fig. 9 is a schematic structural diagram showing an infrared lens according to embodiment 3 of the present invention.

As shown in fig. 9, the infrared lens includes, in order from an object side to an image side, four lenses L1-L4, a first lens L1 having an object side surface S1 and an image side surface S2; the second lens L2 has an object-side surface S3 and an image-side surface S4; the third lens L3 has an object-side surface S5 and an image-side surface S6; the fourth lens L4 has an object-side surface S7 and an image-side surface S8. Optionally, the infrared lens may further include a filter L5 having an object side S9 and an image side S10, and the filter L5 may be a band pass filter. In the infrared lens of the present embodiment, a stop STO may also be provided to adjust the amount of incoming light. The light from the object sequentially passes through the respective surfaces S1 to S10 and is finally imaged on the imaging surface S11.

The effective focal length EFL, the full field angle FOV, the total optical length TTL, the aperture Fno, the surface type, the curvature radius, the thickness, the material and the conic coefficient of the infrared lens in embodiment 3 are shown in table 5:

TABLE 5

As can be seen from table 5, OBJ denotes a light source; the focal length of the infrared lens is f, the focal length of the first lens is f1, and the following relation is satisfied: 3.00< f1/f <4.84, specifically, f1/f 4.838; the total optical length of the infrared lens is TTL, the half-image height of the infrared lens is imgH, and the following relational expression is satisfied: 1.71< TTL/ImgH <1.75, specifically, TTL/ImgH is 1.749; the optical total length of the infrared lens is TTL, the back focal length of the infrared lens is BFL, and the following relational expression is satisfied: 5.29< TTL/BFL <6.24, specifically, TTL/BFL ═ 6.236; the focal length of the infrared lens is f, the focal length of the second lens is f2, and the following relation is satisfied: 2.00< f2/f <7.96, specifically, f2/f 2.207.

the aspheric function relationship of the infrared lens is as follows:

wherein x is the rise of the distance from the aspheric surface vertex to the aspheric surface vertex when the aspheric surface is at the position with the height of h along the optical axis direction; c is the paraxial curvature of the aspheric surface, c being 1/r (i.e., paraxial curvature c is the inverse of radius of curvature r in table 2 above); k is the conic constant (given in table 5 above); ai is a correction coefficient of the i-n th order of the aspherical surface, and the coefficients of the high-order terms a4, a6, A8, a10, a12, a14, and a16 of the respective lens surfaces S1 through S8 are shown in table 6:

TABLE 6

Flour mark

A4

A6

A8

A10

A12

A14

A16

S1

-3.39E-02

-2.08E-04

-8.15E-03

-1.45E-03

7.77E-04

2.27E-04

-3.78E-04

S2

-1.09E-02

-5.80E-03

-1.58E-03

-1.84E-03

-2.62E-05

4.51E-04

-3.22E-04

S3

-6.37E-03

7.02E-03

-3.91E-03

1.48E-03

7.37E-05

-1.81E-04

1.92E-05

S4

-2.94E-02

4.89E-03

3.91E-04

-9.64E-04

1.77E-04

-6.44E-05

6.05E-06

S5

-2.47E-02

-6.77E-03

6.67E-03

-8.23E-03

4.92E-04

1.40E-03

-5.93E-04

S6

-6.53E-02

4.53E-02

-1.48E-02

-2.14E-03

9.49E-04

2.23E-04

-6.26E-05

S7

-1.85E-01

-9.56E-03

1.64E-02

1.37E-03

-7.11E-03

2.97E-03

-3.82E-04

S8

-6.75E-02

-1.29E-02

1.49E-02

-4.39E-03

3.38E-04

5.31E-05

-7.59E-06

As can be seen from tables 5 and 6, in this embodiment, the central thickness of the first lens on the optical axis is CT1, the sum of the central thicknesses of the first to fourth lenses on the optical axis is Σ CT, and the following relationship is satisfied: 0.13< CT1/Σ CT <0.21, specifically, CT1/Σ CT is 0.137; the curvature radius of the object side surface of the second lens is R21, the curvature radius of the image side surface of the second lens is R22, and the following relations are satisfied: 0.47 < R21/R22 < 0.88, specifically, R21/R22 is 0.507; the air space between the first lens and the second lens on the optical axis is AG12, the central thickness of the second lens on the optical axis is CT2, and the following relations are satisfied: 0.43< AG12/CT2<1.01, specifically, AG12/CT2 is 0.570.

Fig. 10 shows a spherical aberration curve of the infrared lens of embodiment 3, which shows that light rays of different aperture angles U intersect the optical axis at different points, and have different deviations from the position of an ideal image point. Fig. 11 shows astigmatism curves of the infrared lens of embodiment 3, which represent meridional field curvature and sagittal field curvature. Fig. 11 shows distortion curves of the infrared lens of embodiment 3, which represent distortion magnitude values in the case of different angles of view. Fig. 12 shows a chromatic aberration of magnification curve of the infrared lens of embodiment 3, which represents a deviation of different image heights on an image plane after light passes through the infrared lens. As can be seen from fig. 10 to 12, the infrared lens according to embodiment 3 can achieve good imaging quality.

Example 4

An infrared lens according to embodiment 4 of the present invention is described below with reference to fig. 13 to 16. Fig. 13 is a schematic structural diagram showing an infrared lens according to embodiment 4 of the present invention.

As shown in fig. 13, the infrared lens includes, in order from an object side to an image side, four lenses L1-L4, a first lens L1 having an object side surface S1 and an image side surface S2; the second lens L2 has an object-side surface S3 and an image-side surface S4; the third lens L3 has an object-side surface S5 and an image-side surface S6; the fourth lens L4 has an object-side surface S7 and an image-side surface S8. Optionally, the infrared lens may further include a filter L5 having an object side S9 and an image side S10, and the filter L5 may be a band pass filter. In the infrared lens of the present embodiment, a stop STO may also be provided to adjust the amount of incoming light. The light from the object sequentially passes through the respective surfaces S1 to S10 and is finally imaged on the imaging surface S11.

The effective focal length EFL, the full field angle FOV, the total optical length TTL, the aperture Fno, the surface type, the curvature radius, the thickness, the material and the conic coefficient of the infrared lens in embodiment 4 are shown in table 7:

TABLE 1

As can be seen from table 7, OBJ denotes a light source; the focal length of the infrared lens is f, the focal length of the first lens is f1, and the following relation is satisfied: 3.00< f1/f <4.84, specifically, f1/f 4.033; the total optical length of the infrared lens is TTL, the half-image height of the infrared lens is imgH, and the following relational expression is satisfied: 1.71< TTL/ImgH <1.75, specifically, TTL/ImgH is 1.726; the optical total length of the infrared lens is TTL, the back focal length of the infrared lens is BFL, and the following relational expression is satisfied: 5.29< TTL/BFL <6.24, specifically, TTL/BFL ═ 5.882; the focal length of the infrared lens is f, the focal length of the second lens is f2, and the following relation is satisfied: 2.00< f2/f <7.96, specifically, f2/f 2.106.

the aspheric function relationship of the infrared lens is as follows:

wherein x is the rise of the distance from the aspheric surface vertex to the aspheric surface vertex when the aspheric surface is at the position with the height of h along the optical axis direction; c is the paraxial curvature of the aspheric surface, c being 1/r (i.e., paraxial curvature c is the inverse of radius of curvature r in table 2 above); k is the conic constant (given in table 7 above); ai is a correction coefficient of the i-n th order of the aspherical surface, and the coefficients of the high-order terms a4, a6, A8, a10, a12, a14, and a16 of the respective lens surfaces S1 through S8 are shown in table 8:

TABLE 8

Flour mark

A4

A6

A8

A10

A12

A14

A16

S1

-3.25E-02

-8.26E-04

-8.12E-03

-1.33E-03

8.52E-04

2.58E-04

-3.65E-04

S2

-1.19E-02

-5.53E-03

-1.59E-03

-1.84E-03

-3.24E-05

4.81E-04

-2.84E-04

S3

-5.19E-03

6.68E-03

-3.85E-03

1.51E-03

8.61E-05

-1.77E-04

2.01E-05

S4

-2.53E-02

5.01E-03

2.93E-04

-9.43E-04

1.94E-04

-5.70E-05

9.94E-06

S5

-2.45E-02

-7.73E-03

6.81E-03

-8.19E-03

4.47E-04

1.36E-03

-6.28E-04

S6

-6.61E-02

4.50E-02

-1.48E-02

-2.14E-03

9.53E-04

2.23E-04

-6.40E-05

S7

-1.86E-01

-1.02E-02

1.65E-02

1.44E-03

-7.09E-03

2.97E-03

-3.84E-04

S8

-6.82E-02

-1.30E-02

1.49E-02

-4.39E-03

3.38E-04

5.30E-05

-7.60E-06

As can be seen from tables 7 and 8, in this embodiment, the central thickness of the first lens on the optical axis is CT1, the sum of the central thicknesses of the first to fourth lenses on the optical axis is Σ CT, and the following relationship is satisfied: 0.13< CT1/Σ CT <0.21, specifically, CT1/Σ CT is 0.176; the curvature radius of the object side surface of the second lens is R21, the curvature radius of the image side surface of the second lens is R22, and the following relations are satisfied: 0.47 < R21/R22 < 0.88, specifically, R21/R22 is 0.484; the air space between the first lens and the second lens on the optical axis is AG12, the central thickness of the second lens on the optical axis is CT2, and the following relations are satisfied: 0.43< AG12/CT2<1.01, specifically, AG12/CT2 is 0.643.

Fig. 14 shows a spherical aberration curve of the infrared lens of embodiment 4, which shows that light rays of different aperture angles U intersect the optical axis at different points, and have different deviations from the position of an ideal image point. Fig. 15 shows astigmatism curves of the infrared lens of embodiment 4, which represent meridional field curvature and sagittal field curvature. Fig. 5 shows distortion curves of the infrared lens of embodiment 4, which represent distortion magnitude values in the case of different viewing angles. Fig. 16 shows a chromatic aberration of magnification curve of the infrared lens of embodiment 4, which represents a deviation of different image heights on an image plane after light passes through the infrared lens. As can be seen from fig. 14 to 16, the infrared lens according to embodiment 4 can achieve good imaging quality.

Example 5

An infrared lens according to embodiment 5 of the present invention is described below with reference to fig. 17 to 20. Fig. 17 is a schematic structural diagram showing an infrared lens according to embodiment 5 of the present invention.

As shown in fig. 17, the infrared lens includes, in order from an object side to an image side, four lenses L1-L4, a first lens L1 having an object side surface S1 and an image side surface S2; the second lens L2 has an object-side surface S3 and an image-side surface S4; the third lens L3 has an object-side surface S5 and an image-side surface S6; the fourth lens L4 has an object-side surface S7 and an image-side surface S8. Optionally, the infrared lens may further include a filter L5 having an object side S9 and an image side S10, and the filter L5 may be a band pass filter. In the infrared lens of the present embodiment, a stop STO may also be provided to adjust the amount of incoming light. The light from the object sequentially passes through the respective surfaces S1 to S10 and is finally imaged on the imaging surface S11.

The effective focal length EFL, the full field angle FOV, the total optical length TTL, the aperture Fno, the surface type, the curvature radius, the thickness, the material and the conic coefficient of the infrared lens in embodiment 5 are shown in table 9:

TABLE 9

As can be seen from table 9, OBJ denotes a light source; the focal length of the infrared lens is f, the focal length of the first lens is f1, and the following relation is satisfied: 3.00< f1/f <4.84, specifically, f1/f 3.020; the total optical length of the infrared lens is TTL, the half-image height of the infrared lens is imgH, and the following relational expression is satisfied: 1.71< TTL/ImgH <1.75, specifically, TTL/ImgH is 1.713; the optical total length of the infrared lens is TTL, the back focal length of the infrared lens is BFL, and the following relational expression is satisfied: 5.29< TTL/BFL <6.24, specifically, TTL/BFL ═ 5.293; the focal length of the infrared lens is f, the focal length of the second lens is f2, and the following relation is satisfied: 2.00< f2/f <7.96, specifically, f2/f 7.957.

the aspheric function relationship of the infrared lens is as follows:

wherein x is the rise of the distance from the aspheric surface vertex to the aspheric surface vertex when the aspheric surface is at the position with the height of h along the optical axis direction; c is the paraxial curvature of the aspheric surface, c being 1/r (i.e., paraxial curvature c is the inverse of radius of curvature r in table 2 above); k is the conic constant (given in table 9 above); ai is a correction coefficient of the i-n th order of the aspherical surface, and the coefficients of the high-order terms a4, a6, A8, a10, a12, a14, and a16 of the respective lens surfaces S1 through S8 are shown in table 10:

watch 10

Flour mark

A4

A6

A8

A10

A12

A14

A16

S1

-3.11E-02

-2.21E-04

-8.20E-03

-1.48E-03

7.29E-04

1.56E-04

-4.43E-04

S2

-8.84E-03

-5.82E-03

-2.22E-03

-2.30E-03

-2.32E-04

4.05E-04

-2.78E-04

S3

-7.03E-03

6.35E-03

-3.55E-03

1.78E-03

1.77E-04

-1.66E-04

2.80E-06

S4

-3.91E-02

3.92E-03

3.30E-04

-1.08E-03

1.08E-04

-2.99E-05

7.05E-05

S5

-2.70E-02

-7.72E-03

6.23E-03

-8.11E-03

5.02E-04

1.37E-03

-6.47E-04

S6

-6.35E-02

4.66E-02

-1.48E-02

-2.28E-03

8.75E-04

2.09E-04

-4.83E-05

S7

-1.81E-01

-1.04E-02

1.60E-02

1.31E-03

-7.10E-03

2.98E-03

-3.78E-04

S8

-6.87E-02

-1.28E-02

1.49E-02

-4.39E-03

3.39E-04

5.32E-05

-7.53E-06

As can be seen from tables 9 and 10, in this embodiment, the central thickness of the first lens on the optical axis is CT1, the sum of the central thicknesses of the first to fourth lenses on the optical axis is Σ CT, and the following relationship is satisfied: 0.13< CT1/Σ CT <0.21, specifically, CT1/Σ CT is 0.203; the curvature radius of the object side surface of the second lens is R21, the curvature radius of the image side surface of the second lens is R22, and the following relations are satisfied: 0.47 < R21/R22 < 0.88, specifically, R21/R22 is 0.878; the air space between the first lens and the second lens on the optical axis is AG12, the central thickness of the second lens on the optical axis is CT2, and the following relations are satisfied: 0.43< AG12/CT2<1.01, specifically, AG12/CT2 ═ 1.004.

Fig. 18 shows a spherical aberration curve of the infrared lens of embodiment 5, which shows that light rays of different aperture angles U intersect the optical axis at different points, with different deviations from the position of an ideal image point. Fig. 19 shows astigmatism curves of the infrared lens of embodiment 5, which represent meridional field curvature and sagittal field curvature. Fig. 19 shows distortion curves of the infrared lens of embodiment 5, which represent distortion magnitude values in the case of different angles of view. Fig. 20 shows a chromatic aberration of magnification curve of the infrared lens of embodiment 5, which represents a deviation of different image heights on an image plane after light passes through the infrared lens. As can be seen from fig. 18 to 20, the infrared lens according to embodiment 5 can achieve good imaging quality.

Example 6

An infrared lens according to embodiment 6 of the present invention is described below with reference to fig. 21 to 24. Fig. 21 is a schematic structural diagram showing an infrared lens according to embodiment 6 of the present invention.

As shown in fig. 21, the infrared lens includes, in order from an object side to an image side, four lenses L1-L4, a first lens L1 having an object side surface S1 and an image side surface S2; the second lens L2 has an object-side surface S3 and an image-side surface S4; the third lens L3 has an object-side surface S5 and an image-side surface S6; the fourth lens L4 has an object-side surface S7 and an image-side surface S8. Optionally, the infrared lens may further include a filter L5 having an object side S9 and an image side S10, and the filter L5 may be a band pass filter. In the infrared lens of the present embodiment, a stop STO may also be provided to adjust the amount of incoming light. The light from the object sequentially passes through the respective surfaces S1 to S10 and is finally imaged on the imaging surface S11.

The effective focal length EFL, the full field angle FOV, the total optical length TTL, the aperture Fno, the surface type, the curvature radius, the thickness, the material and the conic coefficient of the infrared lens in embodiment 6 are shown in table 11:

TABLE 11

As can be seen from table 11, OBJ denotes a light source; the focal length of the infrared lens is f, the focal length of the first lens is f1, and the following relation is satisfied: 3.00< f1/f <4.84, specifically, f1/f 4.221; the total optical length of the infrared lens is TTL, the half-image height of the infrared lens is imgH, and the following relational expression is satisfied: 1.71< TTL/ImgH <1.75, specifically, TTL/ImgH is 1.731; the optical total length of the infrared lens is TTL, the back focal length of the infrared lens is BFL, and the following relational expression is satisfied: 5.29< TTL/BFL <6.24, specifically, TTL/BFL ═ 5.806; the focal length of the infrared lens is f, the focal length of the second lens is f2, and the following relation is satisfied: 2.00< f2/f <7.96, specifically, f2/f 2.254.

the aspheric function relationship of the infrared lens is as follows:

wherein x is the rise of the distance from the aspheric surface vertex to the aspheric surface vertex when the aspheric surface is at the position with the height of h along the optical axis direction; c is the paraxial curvature of the aspheric surface, c being 1/r (i.e., paraxial curvature c is the inverse of radius of curvature r in table 2 above); k is the conic constant (given in table 11 above); ai is a correction coefficient of the i-n th order of the aspherical surface, and the coefficients of the high-order terms a4, a6, A8, a10, a12, a14, and a16 of the respective lens surfaces S1 through S8 are shown in table 12:

TABLE 12

Flour mark

A4

A6

A8

A10

A12

A14

A16

S1

-3.26E-02

-5.70E-04

-8.10E-03

-1.35E-03

8.32E-04

2.47E-04

-3.76E-04

S2

-1.15E-02

-5.36E-03

-1.54E-03

-1.86E-03

-3.11E-05

4.61E-04

-2.98E-04

S3

-6.11E-03

7.07E-03

-3.65E-03

1.58E-03

9.08E-05

-1.86E-04

1.40E-05

S4

-2.89E-02

5.50E-03

3.78E-04

-9.64E-04

2.12E-04

-2.96E-05

3.03E-05

S5

-2.48E-02

-8.17E-03

6.58E-03

-8.14E-03

5.00E-04

1.33E-03

-6.87E-04

S6

-6.64E-02

4.52E-02

-1.49E-02

-2.16E-03

9.42E-04

2.21E-04

-6.42E-05

S7

-1.86E-01

-9.43E-03

1.65E-02

1.39E-03

-7.11E-03

2.97E-03

-3.82E-04

S8

-6.92E-02

-1.30E-02

1.49E-02

-4.39E-03

3.38E-04

5.30E-05

-7.63E-06

As can be seen from tables 11 and 12, in this embodiment, the central thickness of the first lens on the optical axis is CT1, the sum of the central thicknesses of the first to fourth lenses on the optical axis is Σ CT, and the following relationship is satisfied: 0.13< CT1/Σ CT <0.21, specifically, CT1/Σ CT is 0.163; the curvature radius of the object side surface of the second lens is R21, the curvature radius of the image side surface of the second lens is R22, and the following relations are satisfied: 0.47 < R21/R22 < 0.88, specifically, R21/R22 is 0.516; the air space between the first lens and the second lens on the optical axis is AG12, the central thickness of the second lens on the optical axis is CT2, and the following relations are satisfied: 0.43< AG12/CT2<1.01, specifically, AG12/CT2 is 0.438.

Fig. 22 shows a spherical aberration curve of the infrared lens of embodiment 6, which shows that light rays of different aperture angles U intersect the optical axis at different points, with different deviations from the position of an ideal image point. Fig. 23 shows astigmatism curves of the infrared lens of embodiment 6, which represent meridional field curvature and sagittal field curvature. Fig. 23 shows distortion curves of the infrared lens of example 6, which represent distortion magnitude values in the case of different angles of view. Fig. 24 shows a chromatic aberration of magnification curve of the infrared lens of embodiment 6, which represents a deviation of different image heights on an image plane after light passes through the infrared lens. As can be seen from fig. 22 to 24, the infrared lens according to embodiment 6 can achieve good imaging quality.

Example 7

An infrared lens according to embodiment 7 of the present invention is described below with reference to fig. 25 to 28. Fig. 25 is a schematic structural diagram showing an infrared lens according to embodiment 7 of the present invention.

As shown in fig. 25, the infrared lens includes, in order from the object side to the image side, four lenses L1-L4, a first lens L1 having an object side surface S1 and an image side surface S2; the second lens L2 has an object-side surface S3 and an image-side surface S4; the third lens L3 has an object-side surface S5 and an image-side surface S6; the fourth lens L4 has an object-side surface S7 and an image-side surface S8. Optionally, the infrared lens may further include a filter L5 having an object side S9 and an image side S10, and the filter L5 may be a band pass filter. In the infrared lens of the present embodiment, a stop STO may also be provided to adjust the amount of incoming light. The light from the object sequentially passes through the respective surfaces S1 to S10 and is finally imaged on the imaging surface S11.

The effective focal length EFL, the full field angle FOV, the total optical length TTL, the aperture Fno, the surface type, the curvature radius, the thickness, the material and the conic coefficient of the infrared lens according to example 7 are shown in table 13:

watch 13

As can be seen from table 13, OBJ denotes a light source; the focal length of the infrared lens is f, the focal length of the first lens is f1, and the following relation is satisfied: 3.00< f1/f <4.84, specifically, f1/f 3.805; the total optical length of the infrared lens is TTL, the half-image height of the infrared lens is imgH, and the following relational expression is satisfied: 1.71< TTL/ImgH <1.75, specifically, TTL/ImgH is 1.716; the optical total length of the infrared lens is TTL, the back focal length of the infrared lens is BFL, and the following relational expression is satisfied: 5.29< TTL/BFL <6.24, specifically, TTL/BFL ═ 5.586; the focal length of the infrared lens is f, the focal length of the second lens is f2, and the following relation is satisfied: 2.00< f2/f <7.96, specifically, f2/f 2.273.

the aspheric function relationship of the infrared lens is as follows:

wherein x is the rise of the distance from the aspheric surface vertex to the aspheric surface vertex when the aspheric surface is at the position with the height of h along the optical axis direction; c is the paraxial curvature of the aspheric surface, c being 1/r (i.e., paraxial curvature c is the inverse of radius of curvature r in table 2 above); k is the conic constant (given in table 13 above); ai is a correction coefficient of the i-n th order of the aspherical surface, and the coefficients of the high-order terms a4, a6, A8, a10, a12, a14, and a16 of the respective lens surfaces S1 through S8 are shown in table 14:

TABLE 14

As can be seen from tables 13 and 14, in this embodiment, the central thickness of the first lens on the optical axis is CT1, the sum of the central thicknesses of the first to fourth lenses on the optical axis is Σ CT, and the following relationship is satisfied: 0.13< CT1/Σ CT <0.21, specifically, CT1/Σ CT is 0.187; the curvature radius of the object side surface of the second lens is R21, the curvature radius of the image side surface of the second lens is R22, and the following relations are satisfied: 0.47 < R21/R22 < 0.88, specifically, R21/R22 is 0.508; the air space between the first lens and the second lens on the optical axis is AG12, the central thickness of the second lens on the optical axis is CT2, and the following relations are satisfied: 0.43< AG12/CT2<1.01, specifically, AG12/CT2 is 0.816.

Fig. 26 shows a spherical aberration curve of the infrared lens of embodiment 7, which shows that light rays of different aperture angles U intersect the optical axis at different points, with different deviations from the position of an ideal image point. Fig. 27 shows astigmatism curves of the infrared lens of embodiment 7, which represent meridional field curvature and sagittal field curvature. Fig. 27 shows distortion curves of the infrared lens of embodiment 7, which represent distortion magnitude values in the case of different angles of view. Fig. 28 shows a chromatic aberration of magnification curve of the infrared lens of embodiment 7, which represents a deviation of different image heights on an image plane after light passes through the infrared lens. As can be seen from fig. 26 to 28, the infrared lens according to embodiment 7 can achieve good imaging quality.

The invention has the beneficial effects that:

The technical features of the embodiments described above may be arbitrarily combined, and for the sake of brevity, all possible combinations of the technical features in the embodiments described above are not described, but should be considered as being within the scope of the present specification as long as there is no contradiction between the combinations of the technical features.

The above embodiments only express a few embodiments of the present invention, and the description thereof is more specific and detailed, but not construed as limiting the scope of the invention. It should be noted that, for a person skilled in the art, several variations and modifications can be made without departing from the inventive concept, which falls within the scope of the present invention. Therefore, the protection scope of the present patent shall be subject to the appended claims.

Claims

1. An infrared lens, comprising, in order from an object side to an image side: a first lens, a second lens, a third lens and a fourth lens;

the surface of the object side of the first lens is a convex surface, the surface of the image side of the first lens is a concave surface, and the first lens has positive focal power; the surface of the object side of the second lens is a convex surface, the surface of the image side of the second lens is a concave surface, and the second lens has positive focal power; the object side surface of the third lens is a convex surface, and the third lens has positive focal power;

3.00<f1/f<4.84；

the optical total length of the infrared lens is TTL, the back focal length of the infrared lens is BFL, and the following relational expression is satisfied:

5.29<TTL/BFL<6.24。

2. the infrared lens as claimed in claim 1, wherein the radius of curvature of the object-side surface of the second lens is R21, the radius of curvature of the image-side surface of the second lens is R22, and the following relationships are satisfied:

0.47＜R21/R22＜0.88。

3. the infrared lens as claimed in claim 1, wherein the focal length of the infrared lens is f, the focal length of the second lens is f2, and the following relationship is satisfied:

2.00<f2/f<7.96。

4. the infrared lens as claimed in claim 1, wherein the air space between the first and second lenses on the optical axis is AG12, the central thickness of the second lens on the optical axis is CT2, and the following relationship is satisfied:

0.43<AG12/CT2<1.01。

5. the infrared lens as claimed in claim 1, wherein the total optical length of the infrared lens is TTL, the half-image height of the infrared lens is ImgH, and the following relationship is satisfied:

1.71<TTL/ImgH<1.75。

6. the infrared lens as claimed in claim 1, wherein the central thickness of the first lens on the optical axis is CT1, the sum of the central thicknesses of the first to fourth lenses on the optical axis is Σ CT, and the following relationship is satisfied:

0.13<CT1/ΣCT<0.21。