Infrared optical imaging lens, camera module and driver monitor system

Abstract

The disclosure provides an infrared optical imaging lens, a camera module and a DMS. From an object side to an image side along an optical axis, the infrared optical imaging lens sequentially includes a stop, a first lens with a positive refractive power, a second lens with a positive refractive power, a third lens with a negative refractive power, and a filter. An object side surface of the first lens is convex, an image side surface of the first lens is concave. An object side surface of the second lens is concave, an image side surface of the second lens is convex. A paraxial portion of an object side surface of the third lens is convex, and a paraxial portion of an image side surface of the third lens is concave.

Claims

1. An infrared optical imaging lens, from an object side to an image side along an optical axis thereof, sequentially comprising: a stop; a first lens with a positive refractive power, an object side surface of the first lens being convex, an image side surface of the first lens being concave; a second lens with a positive refractive power, an object side surface of the second lens being concave, an image side surface of the second lens being convex; and a third lens with a negative refractive power, a paraxial portion of an object side surface of the third lens being convex, a paraxial portion of an image side surface of the third lens being concave; wherein the first lens is a glass lens, the second lens and the third lens are both plastic aspherical lenses; wherein the infrared optical imaging lens meets the expression: T.sub.L/(IH/tan θ)<1.5, where T.sub.L represents a total optical length of the infrared optical imaging lens, θ represents a half-field of view of the infrared optical imaging lens, IH represents a half image height of the infrared optical imaging lens; wherein the infrared optical imaging lens further meets the expression:
0.16 mm.sup.−1<SD11/IH/SD32<0.19 mm.sup.−1, where SD11 represents a maximum effective radius of the object side surface of the first lens, and SD32 represents a maximum effective radius of the image side surface of the third lens.

2. The infrared optical imaging lens as claimed in claim 1, wherein the infrared optical imaging lens meets the expression:
1<|R11−R12|/CT1<5; where R11 represents a radius of curvature of the object side surface of the first lens, R12 represents a radius of curvature of the image side surface of the first lens, CT1 represents a center thickness of the first lens.

3. The infrared optical imaging lens as claimed in claim 1, wherein the infrared optical imaging lens meets the expression:
0.15<(φ2+φ3)/φ<0.35; where φ2 represents a refractive power of the second lens, φ3 represents a refractive power of the third lens, φ represents a refractive power of the infrared optical imaging lens.

4. The infrared optical imaging lens as claimed in claim 1, wherein the infrared optical imaging lens meets the expression:
0.7<φ1/φ<0.9; where φ1 represents a refractive power of the first lens, φ represents a refractive power of the infrared optical imaging lens.

5. The infrared optical imaging lens as claimed in claim 1, wherein the infrared optical imaging lens meets the expression:
−1.0×10.sup.−6/° C.<(dn/dt)1<3.0×10.sup.−6/° C.; where (dn/dt)1 represents a temperature coefficient of the refractive index of the first lens.

6. The infrared optical imaging lens as claimed in claim 1, wherein the infrared optical imaging lens meets the expression:
−0.3<(R11/R12)−(R22/R21)<0, where R11 represents a radius of curvature of the object side surface of the first lens, R12 represents a radius of curvature of the image side surface of the first lens, R21 represents a radius of curvature of the object side surface of the second lens, R22 represents a radius of curvature of the image side surface of the second lens.

7. The infrared optical imaging lens as claimed in claim 1, wherein the infrared optical imaging lens meets the expression:
SD11/f/tan θ<0.67, where f represents an effective focal length of the infrared optical imaging lens.

8. The infrared optical imaging lens as claimed in claim 1, wherein the infrared optical imaging lens meets the expressions:
n2−n3=0,v2−v3=0; where n2 represents a refractive index of the second lens, n3 represents a refractive index of the third lens, v2 represents a dispersion coefficient of the second lens, and v3 represents a dispersion coefficient of the third lens.

9. The infrared optical imaging lens as claimed in claim 1, wherein an applicable spectral range of the infrared optical imaging lens is 800 nm to 1100 nm.

10. The infrared optical imaging lens as claimed in claim 1, wherein the first lens is a glass aspherical lens.

11. A camera module, comprising a barrel, a holder, an image sensor, and an infrared optical imaging lens, wherein the infrared optical imaging lens is mounted in the barrel, the image sensor is mounted in the holder, and the barrel is movably mounted on the holder, the infrared optical imaging lens is configured to form an optical image, the image sensor is configured to generate image data for the optical image sensed thereby, wherein the infrared optical imaging lens comprising: a stop; a first lens with a positive refractive power, an object side surface of the first lens being convex, an image side surface of the first lens being concave; a second lens with a positive refractive power, an object side surface of the second lens being concave, an image side surface of the second lens being convex; and a third lens with a negative refractive power, a paraxial portion of an object side surface of the third lens being convex, a peripheral portion of the object side surface of the third lens being concave, a paraxial portion of an image side surface of the third lens being concave, a peripheral portion of the image side surface of the third lens being convex; wherein the first lens is a glass lens, the second lens and the third lens are both plastic aspherical lenses; wherein the infrared optical imaging lens meets the expression: T.sub.L/(IH/tan θ)<1.5, where T.sub.L represents a total optical length of the infrared optical imaging lens, θ represents a half-field of view of the infrared optical irriaging lens, IH represents a half image height of the infrared optical imaging lens; wherein the infrared optical imaging lens meets the expressions:
0.15<(φ2+φ3)/φ<0.35; where φ2 represents a refractive power of the second lens, φ3 represents a refractive power of the third lens, φ represents a refractive power of the infrared optical imaging lens.

12. The camera module as claimed in claim 11, wherein the infrared optical imaging lens meets the expressions:
1<|R11−R12|/CT1<5; where R11 represents a radius of curvature of the object side surface of the first lens, R12 represents a radius of curvature of the image side surface of the first lens, CT1 represents a center thickness of the first lens.

13. The camera module as claimed in claim 11, wherein the infrared optical imaging lens meets the expressions:
0.7<φ1/φ<0.9; where φ1 represents a refractive power of the first lens.

14. The camera module as claimed in claim 11, wherein the infrared optical imaging lens meets the expressions:
−1.0×10.sup.−6/° C.<(dn/dt)1<3.0×10.sup.−6/° C.; where (dn/dt)1 represents a temperature coefficient of the refractive index of the first lens material.

15. The camera module as claimed in claim 11, wherein the infrared optical imaging lens meets the expressions:
−0.3<(R11/R12)−(R22/R21)<0, where R11 represents a radius of curvature of the object side surface of the first lens, R12 represents a radius of curvature of the image side surface of the first lens, R21 represents a radius of curvature of the object side surface of the second lens, R22 represents a radius of curvature of the image side surface of the second lens.

16. The camera module as claimed in claim 11, wherein the infrared optical imaging lens meets the expressions:
SD11/f/tan θ<0.67, n2−n3=0,v2−v3=0; where SD11 represents a maximum effective radius of the first lens object side, f represents an effective focal length of the infrared optical imaging lens, n2 represents a refractive index of the second lens, n3 represents a refractive index of the third lens, v2 represents a dispersion coefficient of the second lens, and v3 represents a dispersion coefficient of the third lens.

17. A driver monitor system, comprising a memory, a processor, and a camera module, the memory and the camera module being electrically connected with the processor, the memory being configured to store image data, the processor being configured to process the image data, the camera module comprising an infrared optical imaging lens and an image sensor, the image sensor being opposite to the infrared optical imaging lens and configured to sense and generate the image data, the infrared optical imaging lens sequentially comprising; a stop; a first lens with a positive refractive power, an object side surface of the first lens being convex, an image side surface of the first lens being concave; a second lens with a positive refractive power, an object side surface of the second lens being concave, an image side surface of the second lens being convex; and a third lens with a negative refractive power, a paraxial portion of an object side surface of the third lens being convex, a paraxial portion of an image side surface of the third lens being concave; wherein the first lens is a glass lens, the second lens and the third lens are both plastic aspherical lenses; wherein the infrared optical imaging lens meets the expressions:
T.sub.L/(IH/tan θ)<1.5,
1<|R11−R12|/CT1<5;
0.15<(φ2+φ3)/φ<0.35;
0.7<φ1/φ<0.9; where T.sub.L represents a total optical length of the infrared optical imaging lens, θ represents a half-field of view of the infrared optical imaging lens, IH represents a half image height of the infrared optical imaging lens, R11 represents a radius of curvature of the object side surface of the first lens, R12 represents a radius of curvature of the image side surface of the first lens, CT1 represents a center thickness of the first lens, φ1 represents a refractive power of the first lens, φ2 represents a refractive power of the second lens, φ3 represents a refractive power of the third lens, φ represents a refractive power of the infrared optical imaging lens.

Description

BRIEF DESCRIPTION OF THE DRAWINGS

(1) FIG. 1 is a schematic structural diagram of an infrared optical imaging lens in a first embodiment of the disclosure;

(2) FIG. 2 is a diagram showing field curvature curves of the infrared optical imaging lens in the first embodiment of the disclosure;

(3) FIG. 3 is a diagram showing f-tan θ distortion curves of the infrared optical imaging lens in the first embodiment of the disclosure;

(4) FIG. 4 is a diagram showing longitudinal aberration curves of the infrared optical imaging lens in the first embodiment of the disclosure;

(5) FIG. 5 is a diagram showing lateral chromatic aberration curves of the infrared optical imaging lens in the first embodiment of the disclosure;

(6) FIG. 6 is a diagram showing field curvature curves of the infrared optical imaging lens in a second embodiment of the disclosure;

(7) FIG. 7 is a diagram showing f-tan θ distortion curves of the infrared optical imaging lens in the second embodiment of the disclosure;

(8) FIG. 8 is a diagram showing longitudinal aberration curves of the infrared optical imaging lens in the second embodiment of the disclosure;

(9) FIG. 9 is a diagram showing lateral chromatic aberration curves of the infrared optical imaging lens in the second embodiment of the disclosure;

(10) FIG. 10 is a schematic structural diagram of an infrared optical imaging lens in a third embodiment of the disclosure.

(11) FIG. 11 is a diagram showing field curvature curves of the infrared optical imaging lens in the third embodiment of the disclosure.

(12) FIG. 12 is a diagram showing f-tan θ distortion curves of the infrared optical imaging lens in the third embodiment of the disclosure;

(13) FIG. 13 is a diagram showing longitudinal aberration curves of the infrared optical imaging lens hi the third embodiment of the disclosure;

(14) FIG. 14 is a diagram showing lateral chromatic aberration curves of the infrared optical imaging lens in the third embodiment of the disclosure;

(15) FIG. 15 is a diagram showing field curvature curves of the infrared optical imaging lens in a fourth embodiment of the disclosure.

(16) FIG. 16 is a diagram showing f-tan θ distortion curves of the infrared optical imaging lens in the fourth embodiment of the disclosure;

(17) FIG. 17 is a diagram showing longitudinal aberration craves of the infrared optical imaging lens in the fourth embodiment of the disclosure;

(18) FIG. 18 is a diagram showing lateral chromatic aberration curves of the infrared optical imaging lens in the fourth embodiment of the disclosure;

(19) FIG. 19 is a schematic structural diagram of an imaging device in a fifth embodiment of the disclosure.

(20) FIG. 20 is a schematic structural diagram showing a cross-section of a camera module according to a sixth embodiment of the disclosure.

(21) FIG. 21 is a schematic block diagram of a DMS according to a seventh embodiment of the disclosure.

(22) FIG. 22 is a schematic diagram of the DMS according to the seventh embodiment of the disclosure.

MAIN REFERENCE NUMERALS

(23) TABLE-US-00001 Infrared optical imaging lens 100, 200 Imaging device 300 First lens L1 Second lens L2 Third lens L3 Stop ST Filter G-1 Flat glass G2 Object side surface of the first lens S1 Image side surface of the first lens S2 Object side surface of the second lens S3 Image side surface of the second lens S4 Object side surface of the third lens S5 Image side surface of the third lens S6 Object side surface of the filter S7 Image side surface of the filter S8 Object side surface of the flat glass S9 Image side surface of the flat glass S10 Imaging surface S11 Imaging element 310 Camera module 400 Barrel 401 Holder 402 Image sensor 403 Printed circuit board 404 DMS 500 Memory 501 Processor 502 Car 600

(24) The following embodiments will further illustrate the present disclosure with reference to the above drawings.

DETAILED DESCRIPTION OF PREFERRED EMBODIMENTS

(25) In order to facilitate a better understanding of the present disclosure, the present disclosure will be further explained below with reference to the accompanying drawings. The embodiments of the present disclosure are shown in the drawings, but the present disclosure is not limited to the above-mentioned preferred embodiments. In the contrary, these embodiments are provided to make the disclosure more sufficient.

(26) The disclosure provides an infrared optical imaging lens. From an object side to an image side along an optical axis of the lens, the lens sequentially includes: a stop, a first lens with a positive refractive power, a second lens with a positive refractive power, a third lens with a negative refractive power, and a filter. An object side surface of the first lens is convex, an image side surface of the first lens is concave, an object side surface of the second lens is concave, an image side surface of the second lens is convex. A paraxial portion of an object side surface of the third lens is convex, and a paraxial portion of an image side surface of the third lens is concave. The first lens is a glass lens, the second lens and the third lens are both plastic aspherical lenses. The infrared optical imaging lens meets the expression: T.sub.L/(IH/tan θ)<1.5, where T.sub.L represents a total optical length of the infrared optical imaging lens, θ represents the half-field of view of the infrared optical imaging lens, IH represents the half image height of the infrared optical imaging lens. This expression indicates that when the relationship between the half field angle and the half image height is certain, the infrared optical imaging lens has a smaller total optical length which reduce the volume of the lens effectively.

(27) The stop is configured to limit a diameter of the aperture. The stop is arranged before the first lens in the disclosure, it makes the position of entrance pupil move forward thereby eliminating the influence of the stop on the distortion. The first lens is mainly used for light collection, the second lens is mainly used to correct the field curvature and the astigmatism, and the third lens is mainly used to correct aberrations such as the astigmatism and the distortion, as well as to realize the control of the light exit angle. The use of the plastic aspheric lenses can effectively correct the spherical aberration, reduce the total optical length, reduce the volume of the lens, and realize the miniaturization of the lens.

(28) In some embodiments, the infrared optical imaging lens meets the expression:
1<|R11−R12|/CT1<5;  (1)

(29) where R11 represents a radius of curvature of the object side surface of the first lens, R12 represents a radius of curvature of the image side surface of the first lens, CT1 represents a center thickness of the first lens. Satisfying the expression (1) can effectively improve the ma chi suability of the first lens and make it easy to assemble.

(30) In some embodiments, the infrared optical imaging lens meets the expression:
0.15<(φ2+φ3)/φ<0.35;  (2)

(31) where φ2 represents a refractive power of the second lens, φ3 represents a refractive power of the third lens, φ represents a refractive power of the infrared optical imaging lens. Satisfying the expression (2) can effectively correct the field curvature of the infrared optical imaging lens and improve the resolution of the infrared optical imaging lens.

(32) In some embodiments, the infrared optical imaging lens meets the expression:
0.7<φ1/φ<0.9;  (3)

(33) where φ1 represents a refractive power of the first lens, φ represents a refractive power of the infrared optical imaging lens. The ratio of the refractive power of the first lens to the refractive power of the infrared optical imaging lens satisfies the above expression (3), winch can effectively correct the astigmatism of the infrared optical imaging lens and improve the resolution of the infrared optical imaging lens.

(34) In some embodiments, the infrared optical imaging lens meets the expression:
−1.0×10.sup.−6/° C.<(dn/dt)1<3.0×10.sup.−6/° C.;  (4)

(35) where (dn/dt)1 represents a temperature coefficient of the refractive index of the first lens material. Satisfying the expression (4) can effectively reduce the sensitivity of the infrared optical imaging lens to the temperature and enhance the stability of the resolution at different temperatures.

(36) In some embodiments, the infrared optical imaging lens meets the expression:
−0.3<(R11/R12)−(R22/R21)<0;  (5)

(37) where R11 represents a radius of curvature of the object side surface of the first lens, R12 represents a radius of curvature of the image side surface of the first lens, R21 represents a radius of curvature of the object side surface of the second lens, R22 represents a radius of curvature of the image side surface of the second lens. When the expression (5) is satisfied, the first lens and the second lens form a symmetrical structure in the imaging system, it can improve system aberrations well.

(38) In some embodiments, the infrared optical imaging lens meets the expression:
SD11/f/tan θ<0.67;  (6)

(39) where SD11 represents the maximum effective radius of the object side surface of the first lens, f represents an effective focal length of the infrared optical imaging lens, and θ represents the half-field of view of the infrared optical imaging lens. When the expression (6) is satisfied, the effective focal length of the system can be achieved while ensuring the aperture of the front-end is small.

(40) In some embodiments, the infrared optical imaging lens meets the expressions:
n2−n3=0,v2−v3=0;  (7)

(41) where n2 represents the refractive index of the second lens, n3 represents the refractive index of the third lens, v2 represents the dispersion coefficient of the second lens, and v3 represents the dispersion coefficient of the third lens. Satisfying this expression (7) can make sure that the second lens and the third lens are made of the same material, avoid some processing and testing problems because of using various materials, effectively reduce the technical input cost in actual production, and meet standards of mass production.

(42) In some embodiments, the infrared optical imaging lens meets the expression:
0.16 mm.sup.−1<SD11/IH/SD32<0.19 mm.sup.−1;  (8)

(43) where SD11 represents the maximum effective radius of object side surface of the first lens, IH represents the half image height of the infrared optical imaging lens, SD32 represents the maximum effective radius of image side surface of the third lens. Satisfying this expression (8) is beneficial to realize the control of the incident angle and the exit angle of the light and to ensure the image height requirements.

(44) In some embodiments, the applicable spectral range of the infrared optical imaging lens is 800 mi to 1100 nm. Conventional lenses are designed to be applicable at the wavelength range of 435 nm˜656 nm (visible light), and have poor resolution at the wavelength range of the infrared light. However, the infrared optical imaging lens provided by the disclosure can clearly linage in the wavelength band of 800 nm˜1100 nm (near infrared region), has good imaging quality under near-infrared light conditions, and can meet the imaging requirements of infrared imaging in the DMS system.

(45) In some embodiments, the first lens is a spherical lens. The first lens adopts a glass spherical lens, and the second lens and the third lens adopt plastic aspherical lenses. The design of combining the glass lens and the plastic lens can effectively reduce the production cost of the infrared optical imaging lens.

(46) In some embodiments, the first lens can also be an aspheric lens, which can improve the imaging quality of the infrared optical imaging lens.

(47) In some embodiments, the present disclosure provides an imaging device. The imaging device includes the infrared optical imaging lens as mentioned in any above embodiments and an imaging element which is used to convert an optical image formed by the infrared optical imaging lens into electrical signals.

(48) The shapes of aspheric surfaces of the lens provided by the embodiments of the present disclosure satisfy the following equation:

(49) $z=\frac{{\mathrm{ch}}^2}{1+\sqrt{1-\left(1+K\right)c^2{h}^2}}+{\mathrm{Bh}}^4+{\mathrm{Ch}}^6+{\mathrm{Dh}}^8+{\mathrm{Eh}}^{10}+{\mathrm{Fh}}^{12}$

(50) where z represents a vector height between a positron on the surface and a vertex of the surface along an optical axis of the lens, c represents a curvature of the vertex of the surface, K is a quadratic surface coefficient, h is a distance between the position on the surface and the optical axis, B is a fourth order surface coefficient, C is a sixth order surface coefficient, D is an eighth order surface coefficient, E is a tenth order surface coefficient, F is a twelfth order surface coefficient.

(51) In each of the following embodiments, the thickness, the radius of curvature, and the material of each lens in the infrared optical imaging lens are different. Details can be referred to parameter tables provided in the following embodiments.

First Embodiment

(52) FIG. 1 illustrates an infrared optical imaging lens 100 including three pieces of lens, according to a first embodiment of the disclosure. From an object side to an image side, the infrared optical imaging lens sequentially includes a stop ST, a first lens L1, a second lens L2, a third lens L3, a filter G1, and a flat glass G2.

(53) The first lens L1 is a glass spherical lens with a positive refractive power, an object side surface SI of the first lens L1 is a convex surface, and an image side surface 82 of the first lens L1 is a concave surface.

(54) The second lens L2 is a plastic aspheric lens with a positive refractive power, an object side surface S3 of the second lens L2 is a concave surface, and an image side surface S4 of the second lens L2 is a convex surface.

(55) The third lens L3 is a plastic aspheric lens with a negative refractive power, a paraxial portion of an object side surface S5 of the third lens L3 is convex, and a paraxial portion of an image side surface S6 of the third lens L3 is concave.

(56) Relevant parameters of every lens of the infrared optical imaging lens 100 are shown in Table 1.

(57) TABLE-US-00002 TABLE 1 Radius of Surface curvature Thickness Refractive Abbe NO. Sign (mm) (mm) index number Object surface — ST Stop — −0.16 S1 First lens L1 2.131 0.93 1.73 54.7 S2 5.982 0.95 S3 Second lens L2 −1.907 0.91 1.64 23.5 S4 −0.969 0.07 S5 Third lens L3 3.596 0.50 1.64 23.5 S6 1.073 0.30 S7 Filter G1 — 0.30 1.52 64.2 S8 — 0.48 S9 Flat glass G2 — 0.40 1.52 64.2 S10 — 0.125 S11 Imaging surface — —

(58) In this embodiment, aspherical parameters of every lens of the infrared optical imaging lens 100 are shown in Table 2.

(59) TABLE-US-00003 TABLE 2 Surface No. K B C D E F S3 −7.705 −0.139 −0.096 0.093 0.043 −0.031 S4 −4.581 −0.257 0.245 −0.206 0.107 −0.018 S5 −1.164 −0.184 0.104 −0.03 3.80E−03 −1.33E−04 S6 −6.765 −0.096 0.039 −9.72E−03 1.10E−03 −5.51E−05

(60) In this embodiment, the curves of the field curvature, the distortion, the longitudinal chromatic aberration and the lateral chromatic aberration are shown in FIG. 2, FIG. 3, FIG. 4, and FIG. 5 respectively. From FIG. 2 to FIG. 5, it is apparent that the field curvature, the distortion, and the chromatic aberration can be well corrected.

(61) It can be seen from FIG. 2 that the field curvature of the infrared optical imaging lens 100 provided in this embodiment does not exceed ±0.05 mm, and the difference between field curvatures respectively in the meridian direction and the sagittal direction at the same wavelength does not exceed 0.08 mm. This indicates the field curvature is well corrected.

(62) It can be seen from FIG. 3 that the absolute value of the optical distortion of the infrared optical imaging lens 100 provided in this embodiment is less than 2% in the entire field of view. It indicates that the distortion is well corrected, so that captured images have too slight distortion and are not required to be corrected in digital.

(63) It can be seen from FIG. 4 that the longitudinal chromatic aberration of the infrared optical imaging lens 100 provided by this embodiment is within ±0.05 mm in the entire field of view. Three curves from the negative axis direction to the positive axis direction illustrated in FIG. 4 respectively correspond to the longitudinal chromatic aberration curves of the infrared optical imaging lens 100 at the wavelength of 920 nm, 940 nm, and 960 nm.

(64) It can be seen from FIG. 5 that the lateral chromatic aberration in the wavelength range from 920 to 960 run of the infrared optical imaging lens 100 provided in this embodiment is less than 1.0 μm in the entire field of view, and the difference of vertical axis chromatic aberrations at different wavelengths is very small. This indicates the chromatic aberration of the lens at the near-infrared wavelength band is well corrected.

Embodiment 2

(65) An infrared optical imaging lens of this embodiment is substantially similar to the infrared optical imaging lens 100 of the first embodiment, except that the radius of curvature and the material of each lens in this embodiment are different from that of the first embodiment.

(66) Relevant parameters of event lens of the infrared optical imaging lens provided in this embodiment are shown in Table 3.

(67) TABLE-US-00004 TABLE 3 Radius of Surface curvature Thickness Refractive Abbe NO. Sign (mm) (mm) index number Object surface — ST Stop — −0.15 S1 First lens L1 2.304 1.20 1.73 54.7 S2 6.706 0.77 S3 Second lens L2 −1.774 0.85 1.54 56.0 S4 −1.069 0.14 S5 Third lens L3 2.044 0.50 1.54 56.0 S6 1.050 0.50 S7 Filter G1 — 0.30 1.52 64.2 S8 — 0.28 S9 Flat glass G2 — 0.40 1.52 64.2 S10 — 0.125 S11 Imaging surface — —

(68) In this embodiment, aspherical parameters of every lens of the optical imaging lens provided in this embodiment are shown in Table 4.

(69) TABLE-US-00005 TABLE 4 Surface No. K B C D E F S3 −4.813 −0.119 −0.078 0.089 0.037 −0.028 S4 −4.472 −0.27 0.244 −0.197 0.109 −0.02  S5 −2.29 −0.193 0.102 −0.03 3.96E−03 −1.67E−04 S6 −4.316 −0.1 0.039 −0.01 1.15E−03 −4.92E−05

(70) In this embodiment, the curves of the field curvature, the distortion, the longitudinal chromatic aberration and the lateral chromatic aberration are shown in FIG. 6, FIG. 7, FIG. 8 and FIG. 9, respectively. Three curves from the negative axis direction to the positive axis direction illustrated in FIG. 8 respectively correspond to the longitudinal chromatic aberration curves of the infrared optical imaging lens 100 at the wavelength of 920 nm, 940 nm, and 960 nm. From FIG. 6 to FIG. 9, it is apparent that the field curvature, the distortion, and the chromatic aberration can be well corrected.

Embodiment 3

(71) FIG. 10 illustrates a schematic structural diagram of an infrared optical imaging lens 200 in a third embodiment of the disclosure. The structure of the infrared optical imaging lens 200 in this embodiment is similar to that of the infrared optical imaging lens 100 in the first embodiment except the following differences: the first lens L1 of the optical imaging lens 200 in this embodiment is a glass aspheric lens, the shape of the third lens L3 is different, and the radius of curvature and material selection of each lens are different from that of the first embodiment.

(72) Relevant parameters of every lens of the infrared optical imaging lens 200 provided in this embodiment are shown in Table 5.

(73) TABLE-US-00006 TABLE 5 Radius of Surface curvature Thickness Refractive Abbe NO. Sign (mm) (mm) Index number Object surface — ST Stop — −0.21 S1 First lens L1 1.744 1.25 1.59 67.0 S2 3.630 0.78 S3 Second lens L2 −1.767 0.79 1.64 23.5 S4 −0.870 0.06 S5 Third lens L3 3.636 0.50 1.64 23.5 S6 1.039 0.4 S7 Filter G1 — 0.30 1.52 64.2 S8 — 0.38 S9 Flat glass G2 — 0.40 1.52 64.2 S10 — 0.125 S11 Imaging surface — —

(74) In this embodiment, aspherical parameters of every lens of the optical imaging lens provided in this embodiment are shown in Table 6.

(75) TABLE-US-00007 TABLE 6 Surface No. K B C D E F S1 0 3.61E−03 9.34E−03 −0.018 0.024 −0.011 S2 0 0.036 0.048 −0.054 0.08 −0.021 S3 −4.257 −0.173 −0.027 −0.024 0.09 −0.012 S4 −3.782 −0.268 0.209 −0.181 0.09 −0.014 S5 0.371 −0.141 0.086 −0.027 3.79E−03 −1.83E−04 S6 −6.861 −0.076 0.031 −6.13E−03 2.46E−04   2.95E−05

(76) In this embodiment, the curves of the field curvature, the distortion, the longitudinal chromatic aberration and the lateral chromatic aberration are shown in FIG. 11, FIG. 12, FIG. 13 and FIG. 14, respectively. Three curves from the negative axis direction to the positive axis direction illustrated in FIG. 13 respectively correspond to the longitudinal chromatic aberration curves of the infrared optical imaging lens 200 at the wavelength of 920 nm, 940 nm, and 960 nm. From FIG. 1I to FIG. 14, it is apparent that the field curvature, the distortion, and the chromatic aberration can be well corrected.

Embodiment 4

(77) An infrared optical imaging lens of this embodiment is substantially similar to the infrared optical imaging lens 100 of the first embodiment, except for the following differences: the first lens L1 of the infrared optical imaging lens in this embodiment is a glass aspheric lens, and the radius of curvature and material selection of each lens in the infrared optical imaging lens provided in this embodiment are different from that of the first embodiment.

(78) Relevant parameters of every lens in the infrared optical imaging lens in this embodiment are shown in Tables 7.

(79) TABLE-US-00008 TABLE 7 Radius of Surface curvature Thickness Refractive Abbe NO. Sign (mm) (mm) index number Object surface — ST Stop — −0.20 S1 First lens L1 1.683 1.34 1.53 70.3 S2 4.361 0.83 S3 Second lens L2 −1.393 0.60 1.66 20.9 S4 0.806 0.04 S5 Third lens L3 4.848 0.59 1.66 20.9 S6 1.173 0.4 S7 Filter G1 — 0.30 1.52 64.2 S8 — 0.34 S9 Flat glass G2 — 0.40 1.52 64.2 S10 — 0.125 S11 Imaging surface — —

(80) In this embodiment, aspherical parameters of every lens of the infrared optical imaging lens provided in this embodiment are shown in Table 8.

(81) TABLE-US-00009 TABLE 8 Surface No. K B C D E F S1 0 3.27E−03 −2.64E−03   6.87E−03 −3.47E−03 0 S2 0 0.034 0.041 −0.017 0.021 0 S3 −9.552 −0.514 0.465 −0.6 0.611 −0.216 S4 −4.03 −0.443 0.53 −0.603 0.389 −0.091 S5 −30.717 −0.017 0.023 −9.44E−03   1.61E−03 −9.66E−05

(82) In this embodiment, the curves of the field curvature, the distortion, the longitudinal chromatic aberration and the lateral chromatic aberration are shown in FIG. 15, FIG. 16. FIG. 17 and FIG. 18, respectively. Three curves from the negative axis direction to the positive axis direction illustrated in FIG. 17 respectively correspond to the longitudinal chromatic aberration curves of the infrared optical imaging lens 200 at the wavelength of 920 nm, 940 nm, and 960 nm. From FIG. 15 to FIG. 18, it is apparent that the field curvature, the distortion, and the chromatic aberration can be well corrected.

(83) Table 9 shows the optical characteristics corresponding to the infrared optical imaging lens in the above four embodiments, including the focal length f, the aperture number Fno, and the field of view 20, the total optical length T.sub.L, and the value corresponding to each of the above conditional expression.

(84) TABLE-US-00010 TABLE 9 Embodiment 1 2 3 4 f(mm) 3.60 3.54 3.56 3.57 Fno 1.99 2.01 2.01 2.01 2θ 66.3° 66.6° 67.2° 66.0° T.sub.L(mm) 4.95 5.06 4.98 4.96 T.sub.L*tan θ/IH 1.441 1.471 1.436 1.438 |R11-R12|/CT1 4.156 3.684 1.514 1.995 (φ2 + φ3)/φ 0.199 0.277 0.314 0.276 φ1/φ 0.856 0.804 0.770 0.789 (dn/dt)1 2.8 × 10.sup.−6/° C. 2.8 × 10.sup.−6/° C. −0.7 × 10.sup.−6/° C. 2.0 × 10.sup.−6/° C. (R11/R12)-(R22/R21) −0.152 −0.259 −0.012 −0.192 SD11/f/tan θ 0.653 0.657 0.664 0.649 n2-n3 0 0 0 0 v2-v3 0 0 0 0 SD11/IH/SD32 0.182 0.178 0.170 0.176

(85) Based on the foregoing embodiments, the infrared optical imaging lenses provided by the disclosure have reached the following optical indicators: (1) total optical length: T.sub.L<5.1 mm; (2) applicable spectral range: 800 nm˜1100 nm.

(86) Based on the above embodiments, the infrared optical imaging lens provided by the disclosure has the following advantages:

(87) (1) The infrared optical imaging lens provided by the disclosure adopts the design of three glass-plastic hybrid lenses, realizes the lens miniaturization through a reasonable combination of refractive power and reduces the manufacturing cost.

(88) (2) The design wavelength of conventional lenses is at the range of 435˜656 nm, which is the wavelength of visible light, so the conventional lenses have poor resolution in infrared. The infrared optical imaging lens provided by the disclosure can be clearly imaged in the 800 nm˜1100 nm (near infrared region) waveband with good imaging quality, which can meet the requirements of infrared imaging characteristics and high imaging quality in DMS systems.

Embodiment 5

(89) Please refer to FIG. 19, it is a schematic structural diagram of an imaging device 300 provided by the embodiment. The imaging device 300 includes an imaging element 310 and the infrared optical imaging lens in any of the foregoing embodiments, e.g., the infrared optical imaging lens 100 of the first embodiment. The imaging element 310 can be a Complementary Metal Oxide (CMOS) image sensor or a Charge Coupled Device Semiconductor (CCD) image sensor.

(90) The imaging device 300 can be a sport camera, a panoramic camera, a driving recorder, a surveillance camera, a DMS camera, or any other form of electronic device equipped with an infrared optical imaging lens.

(91) The imaging device 300 provided in this embodiment includes the infrared optical imaging lens 100. Not only the infrared optical imaging lens has the advantages of small size and low cost, but also has good imaging quality under near-infrared light conditions and can provide higher quality imaging performance. Therefore, the imaging device 300 has the advantages of small size, low cost, and good imaging quality under near-infrared light conditions.

Embodiment 6

(92) FIG. 20 illustrates a structural diagram of a camera module 400. The camera module 400 includes a barrel 401, a holder 402, an image sensor 403, a printed circuit board 404, and the infrared optical imaging lens of any one of the foregoing embodiments. FIG. 20 hikes the infrared optical imaging lens 100 of the first embodiment as an example. The infrared optical imaging lens 100 is mounted in the barrel 401, the image sensor 403 is mounted in the holder 402, and the barrel 401 is movably mounted on the holder 402. The infrared optical imaging lens 100 is configured to form an optical image. The image sensor 403 is opposite to the infrared optical imaging lens 100 and is configured to generate image data for the optical image sensed thereby. The image sensor 403 may be a CMOS sensor or a CCD sensor.

(93) It is noted that the image sensor 403 may be mounted on the printed circuit board 404, or may be electrically connected with a processing chip, to process the image data.

Embodiment 7

(94) FIG. 21 is a block diagram of a DMS 500 provided in this embodiment. The DMS 500 includes a memory 501, a processor 502, and the camera module 400 as described above. The memory 501 and the camera module 400 are both electrically connected with the processor 502. The camera module 400 is configured to capture images, the processor 502 is configured to acquire and process image data of the captured images, the memory 501 is configured to store the image data of the captured images. As illustrated in FIG. 22, the DMA 500 is installed in a car 600, and is configured to monitor the driver, thereby ensuring the safety of the driving.

(95) The above embodiments just describe some implementation manners of the disclosure, the descriptions are specific and detailed, but cannot be understood as limiting the scope of the application. It should be noted that, for those of ordinary skill in the art, without departing from the concept of the application, modifications and improvements can be made, which should belong to the protection scope of the application. Therefore, the protection scope of this application should be subject to the appended claims.