TWM510465U - Photographing optical lens assembly - Google Patents

Description

Optical camera lens

The present invention relates to an optical lens, and more particularly to an optical imaging lens.

In recent years, the popularity of portable electronic products such as mobile phones and digital cameras has led to the development of image module related technologies. The image module mainly includes an optical camera lens, a module holder unit and a sensor. And other components, and the thin and light trend of mobile phones and digital cameras also make the demand for miniaturization of image modules higher and higher, with the charge coupled device (Charge Coupled Device, CCD for short) or complementary metal oxide semiconductor components (Complementary) Metal-Oxide Semiconductor (referred to as CMOS) technology advancement and downsizing, the optical camera lens mounted in the image module also needs to be shortened accordingly, but in order to avoid the photographic effect and quality degradation, shorten the length of the optical camera lens It is still necessary to balance good optical performance.

In addition, the above-mentioned photosensitive coupling element or complementary metal oxide semiconductor element can be reduced in size by pixels, so that a higher pixel can be achieved in the same area, but the smaller the pixel, the lower the amount of light entering the system, which causes the noise to increase and affects the image. quality. Therefore, the lens must increase the amount of light entering, reducing noise generation to maintain image quality.

Therefore, how to produce an optical camera lens that meets the above requirements and continuously improve its image quality has long been a eagerly pursued goal in the field of production, official and academic circles.

The object of the present invention is to provide an imaging lens with a wide-angle and large aperture, which can simultaneously have high resolution and high manufacturability under the condition that the lens system is thinned.

The optical lens of the present invention includes a first lens, an aperture, a second lens, a third lens, a fourth lens, a fifth lens, and a first step along an optical axis from the object side to the image side. And a sixth lens, wherein the first lens to the sixth lens respectively comprise an object side facing the object side and passing the imaging light and an image side facing the image side and passing the imaging light.

The second lens has a negative refractive power and a concave side of the image side. The fourth lens has a positive refractive power. The fifth lens has a positive refractive power. The image side surface of the sixth lens is a concave surface.

Among them, the optical imaging lens has only six lenses with refractive power. The radius of curvature of the object side surface of the fourth lens is R7, and the radius of curvature of the image side surface of the fourth lens is R8, and satisfies -14.97<R7/R8<-0.12.

With the above description, the novel optical imaging lens can effectively correct the system aberration and coma of the lens, and can maintain the high light input amount while shortening the system length of the lens.

10‧‧‧Optical camera lens

62‧‧‧like side

2‧‧‧ aperture

7‧‧‧ fifth lens

3‧‧‧first lens

71‧‧‧ ‧ side

31‧‧‧ ‧ side

72‧‧‧like side

32‧‧‧like side

8‧‧‧ sixth lens

4‧‧‧second lens

81‧‧‧ ‧ side

41‧‧‧ ‧ side

82‧‧‧like side

42‧‧‧like side

9‧‧‧Filter

5‧‧‧ third lens

91‧‧‧ ‧ side

51‧‧‧ ‧ side

92‧‧‧like side

52‧‧‧like side

100‧‧‧ imaging surface

6‧‧‧Fourth lens

I‧‧‧ optical axis

61‧‧‧ ‧ side

Other features and effects of the present invention will be apparent from the detailed description of the embodiments referring to the drawings, wherein: 1 is a schematic view showing a first embodiment of the optical imaging lens of the present invention; FIG. 2 is an aberration diagram of the first embodiment; FIG. 3 is a table showing the optical of the first embodiment. Figure 4 is a table showing the aspherical coefficients of the lenses of the first embodiment; Figure 5 is a schematic view showing a second embodiment of the novel optical imaging lens; Figure 6 is the second embodiment Various aberration diagrams of the example; FIG. 7 is a table diagram illustrating optical data of the second embodiment; FIG. 8 is a table diagram illustrating aspherical coefficients of the lenses of the second embodiment; FIG. FIG. 10 is a third embodiment of the present invention; FIG. 10 is a partial diagram showing the optical data of the third embodiment; FIG. 11 is a table diagram illustrating the optical data of the third embodiment; Is a table diagram illustrating the aspherical coefficients of the lenses of the third embodiment; FIG. 13 is a schematic view showing a fourth embodiment of the novel optical imaging lens; FIG. 14 is a fourth embodiment of the fourth embodiment. Aberration map; Figure 15 is a table diagram illustrating the fourth real Embodiment of the optical data; FIG. 16 is a table diagram illustrating aspherical coefficients of each lens of the fourth embodiment of the embodiment; Figure 17 is a schematic view showing a fifth embodiment of the optical pickup lens of the present invention; Figure 18 is a diagram showing aberrations of the fifth embodiment; Figure 19 is a table showing the optical body of the fifth embodiment Figure 20 is a table showing the aspherical coefficients of the lenses of the fifth embodiment; Figure 21 is a schematic view showing a sixth embodiment of the novel optical imaging lens; Figure 22 is the sixth embodiment FIG. 23 is a table showing the optical data of the sixth embodiment; FIG. 24 is a table showing the aspherical coefficients of the lenses of the sixth embodiment; and FIG. 25 is A table diagram illustrating the optical parameter relationship of the first embodiment to the sixth embodiment of the optical imaging lens.

Before the present invention is described in detail, it should be noted that in the following description, similar elements are denoted by the same reference numerals.

Referring to FIG. 1 , a first embodiment of the optical imaging lens 10 of the present invention includes a first lens 3 , an aperture 2 , a second lens 4 , and a third lens 5 along the optical axis I from the object side to the image side. A fourth lens 6, a fifth lens 7, a sixth lens 8, and a filter 9. When light enters the optical imaging lens 10 and passes through the first lens 3, the aperture 2, the second lens 4, the third lens 5, the fourth lens 6, the fifth lens 7, and the sixth lens 8 And the filter 9 is formed on the imaging plane 100 (Image Plane) An image. The filter 9 is an IR Cut Filter for preventing infrared light from being transmitted to the imaging surface 100 to affect imaging quality.

The first lens 3, the second lens 4, the third lens 5, the fourth lens 6, the fifth lens 7, the sixth lens 8, and the filter 9 each have an orientation. The side faces 31, 41, 51, 61, 71, 81, 91 through which the imaging light passes, and the image side faces 32, 42, 52, 62, 72, 82, 92 which face the image side and allow imaging light to pass therethrough. It is added that the object side is the side facing the object to be photographed, and the image side is the side facing the image forming surface 100. The side surfaces 31, 41, 51, 61, 71, 81 and the image side surfaces 32, 42, 52, 62, 72, 82 are all aspherical.

In addition, in order to meet the demand for light weight of the product, the first lens 3 to the sixth lens 8 are both made of a refractive power and are made of a plastic material, but the material is not limited thereto.

The object side surface of the following lens is called a concave surface when it is concave toward the object side in the vicinity of the optical axis I, and is called a convex surface when it is concave toward the image side, and the convex side of the image side surface of the lens in the vicinity of the optical axis I is called convex surface. If it is concave toward the image side, it is called a concave surface.

The first lens 3 has a positive refractive power. The object side surface 31 of the first lens 3 is a convex surface, and the image side surface 32 of the first lens 3 is a convex surface.

The second lens 4 has a negative refractive power. The object side surface 41 of the second lens 4 is a convex surface, and the image side surface 42 of the second lens 4 is a concave surface.

The third lens 5 has a negative refractive power, the object side surface 51 of the third lens 5 is a convex surface, and the image side surface 52 of the third lens 5 is a concave surface.

This fourth lens 6 has a positive refractive power. The fourth lens 6 The object side surface 61 is a convex surface, and the image side surface 62 of the fourth lens 6 is a convex surface.

This fifth lens 7 has a positive refractive power. The object side surface 71 of the fifth lens 7 is convex and has an inflection point, and the image side surface 72 of the fifth lens 7 is a convex surface.

The sixth lens 8 has a negative refractive power. The object side surface 81 of the sixth lens 8 is a concave surface, and the image side surface 82 of the sixth lens 8 is a concave surface and has an inflection point.

In the first embodiment, only the above lens has refractive power.

The other detailed optical data of the first embodiment is as shown in FIG. 3, and the overall system focal length (EFL) of the first embodiment is 4.57 mm, and the half field of view (HFOV) is 33°, the aperture value (Fno) is 2.4, and the system length is 5.5 mm. The length of the system refers to the distance between the object side surface 31 of the first lens 3 and the imaging surface 100 on the optical axis I.

In addition, the aspherical surface change of the present invention is defined by the following formula:

Where: Y: the distance between the point on the aspheric curve and the optical axis I; Z: the depth of the aspheric surface (the point on the aspheric surface from which the optical axis I is Y, and the tangent to the vertex on the aspherical optical axis I, The vertical distance between the two); the radius of curvature of the surface of the R lens; K: the conic constant; a _{2 i} : the 2ith order aspheric coefficient.

The aspherical coefficients of the object side surface 31 of the first lens 3 to the image side surface 82 of the sixth lens 8 in the formula (1) are as shown in FIG. Here, the column number 31 in FIG. 4 indicates that it is the aspherical coefficient of the object side surface 31 of the first lens 3, and the other fields are deduced by analogy.

In addition, the relationship between the important parameters in the first embodiment is as follows: f1/f=0.641, |f2/f1|=1.515, |f3/f4|=2.908, R7/R8=-0.716, R10/ R11=1.105, T4/T6=3.000, T5/T6=3.440, D56/BFL=0.287, SD/TD=0.845.

Wherein f1 is the focal length of the first lens 3; f2 is the focal length of the second lens 4; f3 is the focal length of the third lens 5; f4 is the focal length of the fourth lens 6; f is the optical imaging lens 10 The focal length of the system; R7 is the radius of curvature of the object side surface 61 of the fourth lens 6; R8 is the radius of curvature of the image side surface 62 of the fourth lens 6, R10 is the radius of curvature of the image side surface 72 of the fifth lens 7, R11 is The radius of curvature of the object side surface 81 of the sixth lens 8; T4 is the thickness of the fourth lens 6 on the optical axis I; T5 is the thickness of the fifth lens 7 on the optical axis I; and T6 is the sixth lens 8 a thickness on the optical axis I; D56 is between the fifth lens 7 and the sixth lens 8 on the optical axis I Air gap; BFL is the distance from the image side 82 of the sixth lens 8 to the imaging plane 100 on the optical axis I; SD is the distance of the aperture 2 to the image side 82 of the sixth lens 8 on the optical axis I And TD is the distance of the object side surface 31 of the first lens 3 to the image side surface 82 of the sixth lens 8 on the optical axis I.

Referring again to FIG. 2, the pattern of (a) illustrates the longitudinal chromatic aberration and spherical aberration of the first embodiment on the imaging surface 100, and the pattern of (b) illustrates the first implementation. For example, the astigmatism aberration on the imaging plane 100 with respect to the sagittal direction and the tangential direction, and the pattern of (c) illustrates the lateral chromatic aberration of the first embodiment on the imaging plane 100. (lateral chromatic aberration), the pattern of (d) illustrates the distortion aberration of the first embodiment on the imaging plane 100. The longitudinal chromatic aberration and spherical aberration of the first embodiment are shown in Fig. 2(a), and the curves formed by each of the wavelengths are close to each other and close to the middle, indicating that the light of each wavelength on the axis is concentrated near the imaging point. It can be seen from the deflection amplitude of the curve that the deviation of the imaging point on the axis is controlled within the range of ±0.005 mm, so the embodiment does improve the spherical aberration significantly. In addition, the distances between the three representative wavelengths are also relatively close to each other, representing different wavelengths. The imaging position of the light has been quite concentrated, that is, the axial chromatic aberration has also been significantly improved.

In the astigmatic aberration diagram of Fig. 2(b), the focal length variation of the three representative wavelengths over the entire field of view falls within ±0.01 mm, indicating The optical system of the first embodiment can effectively alleviate astigmatism. In the lateral chromatic aberration diagram of Fig. 2(c), it can be seen from the deflection amplitude of the curve of each wavelength that the principal ray deviation of the off-axis ray is controlled within ±1 μm, indicating the lateral direction of the first embodiment. The color difference has met the imaging quality requirements of the optical system. The distortion aberration diagram of FIG. 2(d) shows that the distortion aberration of the first embodiment is maintained within ±1%, indicating that the distortion aberration of the first embodiment also conforms to the imaging quality of the optical system. It is required that the first embodiment can provide better imaging quality under the condition that the length of the system has been shortened to about 5.5 mm compared with the existing optical lens, so that the first embodiment can maintain good optics. Under the condition of performance, shorten the lens length and expand the shooting angle to achieve a more thin product design.

Referring to FIG. 5, a second embodiment of the optical imaging lens 10 of the present invention is substantially similar to the first embodiment except for each optical data, aspherical coefficient, and the lenses 3, 4, 5, 6, and 7. The parameters of the eight lenses are more or less different, and the object side surface 41 and the image side surface 42 of the second lens 4 are both concave. The third lens 5 has a positive refractive power, and the object side surface 71 of the fifth lens 7 is a concave surface.

The detailed optical data is shown in Fig. 7, and the overall system focal length of the second embodiment is 4.47 mm, the half angle of view (HFOV) is 33, the aperture value (Fno) is 2.4, and the system length is 5.48 mm.

Fig. 8 is an aspherical coefficient of the image side surface 31 of the first lens 3 of the second embodiment to the image side surface 82 of the sixth lens 8.

In addition, the relationship between the important parameters in the optical imaging lens 10 of the second embodiment is as follows: F1/f=0.593, |f2/f1|=1.121, |f3/f4|=3.371, R7/R8=-2.333, R10/R11=1.188, T4/T6=4.080, T5/T6=1.680, D56/BFL =0.183, SD/TD=0.841.

Referring to FIG. 6, the second embodiment can be seen from the longitudinal chromatic aberration of (a) and the spherical aberration, the astigmatic aberration of (b), the lateral chromatic aberration of (c), and the distortion aberration diagram of (d). It also maintains good optical properties.

Referring to FIG. 9, a third embodiment of the optical imaging lens 10 of the present invention is substantially similar to the first embodiment except for each optical data, aspherical coefficient, and the lenses 3, 4, 5, 6, and 7. The parameters of the 8th are more or less different, and the object side surface 41 and the image side surface 42 of the second lens 4 are concave surfaces, the third lens 5 has a positive refractive power, and the object side surface 51 is a concave surface and an image side surface 52 thereof. The convex side, the object side surface 71 of the fifth lens 7 is a concave surface.

The detailed optical data is shown in Fig. 11, and the overall system focal length of the third embodiment is 4.65 mm, the half angle of view (HFOV) is 31.5°, the aperture value (Fno) is 2.35, and the system length is 5.5 mm.

Fig. 12 is an aspherical coefficient of the image side surface 31 of the first lens 3 of the third embodiment to the image side surface 82 of the sixth lens 8.

Further, the relationship between the important parameters in the optical imaging lens 10 of the third embodiment is as follows: f1/f=0.596, |f2/f1|=1.245, |f3/f4|=1.911, R7/R8 =-2.620, R10/R11=1.286, T4/T6=2.480, T5/T6=3.680, D56/BFL=0.127, SD/TD=0.835.

Referring to FIG. 10, the longitudinal chromatic aberration and spherical aberration of (a), the astigmatic aberration of (b), the lateral chromatic aberration of (c), and the distortion aberration diagram of (d) can be seen. The third embodiment also maintains good optical performance.

Referring to FIG. 13, a fourth embodiment of the optical imaging lens 10 of the present invention is substantially similar to the first embodiment except for each optical data, aspherical coefficient, and the lenses 3, 4, 5, 6, and 7. The parameters of the 8th are more or less different, and the object side surface 41 and the image side surface 42 of the second lens 4 are concave surfaces, the third lens 5 has a positive refractive power, and the object side surface 51 is a concave surface and an image side surface 52 thereof. The convex side, the object side surface 71 of the fifth lens 7 is a concave surface.

The detailed optical data is as shown in Fig. 15, and the overall system focal length of the fourth embodiment is 4.65 mm, the half angle of view (HFOV) is 31.8 °, the aperture value (Fno) is 2.35, and the system length is 5.4 mm.

Fig. 16 is an aspherical coefficient of the image side surface 31 of the first lens 3 of the fourth embodiment to the image side surface 82 of the sixth lens 8.

In addition, the relationship between the important parameters in the optical imaging lens 10 of the fourth embodiment is as follows: f1/f=0.578, |f2/f1|=1.230, |f3/f4|=0.950, R7/R8 =-13.607, R10/R11=1.25, T4/T6=2.160, T5/T6=3.240, D56/BFL=0.167, SD/TD=0.813.

Referring to FIG. 14, the fourth embodiment can be seen from the longitudinal chromatic aberration of (a) and the spherical aberration, the astigmatic aberration of (b), the lateral chromatic aberration of (c), and the distortion aberration diagram of (d). It also maintains good optical properties.

Referring to FIG. 17, a fifth embodiment of the optical imaging lens 10 of the present invention is substantially similar to the first embodiment except for each optical data, aspherical coefficient, and the lenses 3, 4, 5, 6, and 7. The parameters of the 8 lenses are more or less different, and the object side 51 and the image side 52 of the third lens 5 are both Concave.

The detailed optical data is shown in Fig. 19, and the overall system focal length of the fifth embodiment is 4.50 mm, the half angle of view (HFOV) is 33°, the aperture value (Fno) is 2.42, and the system length is 5.5 mm.

Fig. 20 is an aspherical coefficient of the image side surface 31 of the first lens 3 of the fifth embodiment to the image side surface 82 of the sixth lens 8.

Further, the relationship between the important parameters in the optical imaging lens 10 of the fifth embodiment is as follows: f1/f=0.656, |f2/f1|=2.251, |f3/f4|=1.219, R7/R8 =-9.200, R10/R11=1.111, T4/T6=3.880, T5/T6=3.640, D56/BFL=0.307, SD/TD=0.819.

Referring to FIG. 18, the fifth embodiment can be seen from the longitudinal chromatic aberration of (a) and the spherical aberration, the astigmatic aberration of (b), the lateral chromatic aberration of (c), and the distortion aberration diagram of (d). It also maintains good optical properties.

Referring to FIG. 21, a sixth embodiment of the optical imaging lens 10 of the present invention is substantially similar to the first embodiment except for each optical data, aspherical coefficient, and the lenses 3, 4, 5, 6, and 7. The parameters of the eight lenses are more or less different, and the object side surface 41 and the image side surface 42 of the second lens 4 are both concave. The third lens 5 has a positive refractive power, and the object side surface 71 of the fifth lens 7 is a concave surface.

The detailed optical data is shown in Fig. 23, and the overall system focal length of the sixth embodiment is 4.47 mm, the half angle of view (HFOV) is 33°, the aperture value (Fno) is 2.3, and the system length is 5.4 mm.

Figure 24 is the object side of the first lens 3 of the sixth embodiment. 31 to aspherical coefficients of the image side surface 82 of the sixth lens 8.

Further, the relationship between the important parameters in the optical imaging lens 10 of the sixth embodiment is as follows: f1/f=0.588, |f2/f1|=1.046, |f3/f4|=2.389, R7/R8 =-0.130, R10/R11=1.063, T4/T6=2.914, T5/T6=1.571, D56/BFL=0.154, SD/TD=0.826.

Referring to FIG. 22, the sixth embodiment can be seen from the longitudinal chromatic aberration of (a) and the spherical aberration, the astigmatic aberration of (b), the lateral chromatic aberration of (c), and the distortion aberration diagram of (d). It also maintains good optical properties.

Referring again to FIG. 25, which is a table diagram of the optical parameter relationships of the above six embodiments, when the relationship between the optical parameters in the optical imaging lens 10 of the present invention satisfies the following conditional formula, the system length is shortened. In this case, there will still be better optical performance, so that when the present invention is applied to a related portable electronic device, a thinner product can be produced:

(1) When 0.52 < f1/f < 0.72 is satisfied, a good balance can be obtained between wide-angle optical characteristics and lens manufacturability, and if f1/f is small, good lens manufacturability can be obtained. When f1/f is large, a wider system field of view angle can be obtained.

(2) When 0.94<|f2/f1|<2.48 is satisfied, the eccentricity sensitivity during lens assembly and the system chromatic aberration of the lens can be reduced, wherein if |f2/f1| is small, the system color difference of the lens A better correction can be obtained. If |f2/f1| is large, the assembly eccentricity sensitivity of the lens can be effectively reduced.

(3) When |f3/f4|<3.71 is satisfied, the system astigmatism and field curvature of the lens can be effectively corrected.

(4) When -14.97<R7/R8<-0.12 is satisfied, the system coma of the lens can be corrected, and the lens length can be effectively shortened while the lens maintains a high amount of light, wherein if R7/R8 is small The system length of the lens can be easily shortened. If the R7/R8 is larger, the lens can obtain a higher amount of light.

(5) When 0.96<R10/R11<1.41 is satisfied, the field curvature can be corrected while maintaining good manufacturability. If R10/R11 is smaller, the eccentricity sensitivity can be reduced, and a higher manufacturing quality can be obtained. Rate, if R10/R11 tends to be large, the field curvature correction effect is better.

(6) When 1.94<T4/T6<4.49 is satisfied, the balance between the system length and manufacturability of the lens can be achieved. If the T4/T6 is small, the sensitivity of the lens can be averaged, so that each single component is It is easy to manufacture, and if T4/T6 is large, the system length of the lens can be effectively shortened, which is advantageous for thinning.

(7) When 1.41<T5/T6<4.05 is satisfied, it can have a relatively stable manufacturing yield under the premise of thinning the lens. If T5/T6 is smaller, the lens can have better moldability and manufacturing. The accuracy is relatively stable. If the T5/T6 is large, the system length of the lens can be effectively shortened.

(8) When the 0.73<SD/TD<0.93 is satisfied, the lens can have high efficiency and high manufacturing yield. If the SD/TD is small, the eccentricity of the most sensitive lens in the lens can be reduced, so that The overall lens yield is effectively controlled. If the SD/TD is large, the angle of view can be increased and the system coma can be effectively corrected.

However, given the unpredictability of optical system design, Under the framework of the present invention, the above conditional expression can better shorten the length of the optical imaging lens 10, increase the amount of light incident (reduced aperture value), increase the angle of view, improve imaging quality, or improve assembly yield. Improve the shortcomings of the prior art.

In summary, the novel optical imaging lens 10 can achieve the following functions and advantages, so that the purpose of the present invention can be achieved:

The first lens 3 has a positive refractive power, and mainly provides the refractive power required for the optical imaging lens 10; the aperture 2 is disposed between the first lens 3 and the second lens 4, and can be manufactured and incident on the lens. A better balance is achieved between the angles of the sensors disposed on the imaging surface 100; the second lens 4 is a negative refractive power; the third lens 5 has an aspherical characteristic, which can better correct the lens at a wide angle and a large aperture. The problem of astigmatism which is easy to occur in the optical system, so that the lens is easy to achieve the effect of large aperture; the fourth lens 6 has a positive refractive power, and can be effectively corrected in accordance with the focal length of the third lens 5 satisfying |f3/f4|<3.71. The system astigmatism and curvature of field of the lens; the fifth lens 7 has a positive refractive power, which can effectively shorten the system length of the lens, and has a surface design of the object side surface 71 of the inflection point 711, which can effectively correct the optical lens of the lens at a large aperture. The system coma generated by the characteristic; the sixth lens 8 can adjust the angle of the light incident on the sensor to achieve the maximum light collecting effect, reduce the chance of the sensor generating noise, and improve the overall image quality, and 81 is a concave side surface concave to the object side, the axial chromatic aberration can be preferably corrected, the center of the lens to improve image quality.

The design of the novel optical imaging lens 10 is shown by the description of the foregoing six embodiments, and the system length of the embodiments can be shortened to Below 5.5mm, compared with the existing optical camera lens, the lens of the present invention can be used to manufacture a thinner product, so that the novel has economic benefits in line with market demand.

However, the above is only the embodiment of the present invention, and when it is not possible to limit the scope of the present invention, all the simple equivalent changes and modifications according to the scope of the patent application and the contents of the patent specification are still This new patent covers the scope.

10‧‧‧Optical camera lens

62‧‧‧like side

2‧‧‧ aperture

7‧‧‧ fifth lens

3‧‧‧first lens

71‧‧‧ ‧ side

31‧‧‧ ‧ side

72‧‧‧like side

32‧‧‧like side

8‧‧‧ sixth lens

4‧‧‧second lens

81‧‧‧ ‧ side

41‧‧‧ ‧ side

82‧‧‧like side

42‧‧‧like side

9‧‧‧Filter

5‧‧‧ third lens

91‧‧‧ ‧ side

51‧‧‧ ‧ side

92‧‧‧like side

52‧‧‧like side

100‧‧‧ imaging surface

6‧‧‧Fourth lens

I‧‧‧ optical axis

61‧‧‧ ‧ side

Claims (23)

An optical imaging lens includes a first lens, an aperture, a second lens, a third lens, a fourth lens, a fifth lens, and a sixth in sequence along an optical axis from the object side to the image side a lens, and the first lens to the sixth lens respectively include an object side facing the object side and passing the imaging light and an image side facing the image side and passing the imaging light; the second lens has a negative refractive power, the second lens The image side of the second lens is a concave surface; the fourth lens has a positive refractive power; the fifth lens has a positive refractive power; the image side of the sixth lens is a concave surface; wherein the optical imaging lens has a refractive power of only six lenses, The radius of curvature of the object side surface of the fourth lens is R7, and the radius of curvature of the image side surface of the fourth lens is R8, and satisfies -14.97 < R7 / R8 < - 0.12. The optical imaging lens of claim 1, wherein at least one of an object side and an image side of the third lens is aspherical. The optical imaging lens of claim 1, wherein the object side of the fifth lens is aspherical and has an inflection point. The optical imaging lens according to claim 3, wherein the object side surface of the fifth lens is a convex surface, and the image side surface of the fifth lens is a convex surface. The optical imaging lens according to claim 1, wherein the object side surface of the fifth lens is a concave surface, and the image side surface of the fifth lens is a convex surface. The optical imaging lens of claim 1, wherein the second lens The sides of the object are convex. The optical imaging lens of claim 1, wherein the object side surface of the second lens is a concave surface. The optical imaging lens according to claim 1, wherein the third lens has a positive refractive power, the object side surface of the third lens is a concave surface, and the image side surface of the third lens is a convex surface. The optical imaging lens of claim 1, wherein the third lens has a positive refractive power, the object side surface of the third lens is a convex surface, and the image side surface of the third lens is a concave surface. The optical imaging lens of claim 1, wherein the third lens has a negative refractive power, the object side surface of the third lens is a convex surface, and the image side surface of the third lens is a concave surface. The optical imaging lens of claim 1, wherein the third lens has a negative refractive power, the object side surface of the third lens is a concave surface, and the image side surface of the third lens is a concave surface. The optical imaging lens of claim 1, wherein the focal length of the optical imaging lens is f, the focal length of the first lens is f1, and 0.52 < f1/f < 0.72 is satisfied. The optical imaging lens of claim 1, wherein the first lens has a focal length of f1, the second lens has a focal length of f2, and satisfies 0.94<|f2/f1|<2.48. The optical imaging lens of claim 1, wherein the focal length of the third lens is f3, the focal length of the fourth lens is f4, and |f3/f4|<3.71 is satisfied. The optical imaging lens of claim 1, wherein the fourth lens is The thickness on the optical axis is T4, and the thickness of the sixth lens on the optical axis is T6, and also satisfies the following conditional formula: 1.94 < T4 / T6 < 4.49. The optical imaging lens according to claim 1, wherein the thickness of the fifth lens on the optical axis is T5, the thickness of the sixth lens on the optical axis is T6, and the following conditional expression is also satisfied: 1.41 < T5/ T6 < 4.05. The optical imaging lens of claim 1, wherein the distance from the aperture to the image side of the sixth lens on the optical axis is SD, and the object side of the first lens to the image side of the sixth lens is on the optical axis. The distance on the upper side is TD, and the following conditional formula is also satisfied: 0.73<SD/TD<0.93. The optical imaging lens according to claim 1, wherein the image side of the fifth lens has a radius of curvature of R10, and the radius of curvature of the object side of the sixth lens is R11, and satisfies the following conditional formula: 0.96<R10/R11 <1.41. An optical imaging lens includes a first lens, an aperture, a second lens, a third lens, a fourth lens, a fifth lens, and a sixth in sequence along an optical axis from the object side to the image side a lens, and the first lens to the sixth lens respectively include an object side facing the object side and passing the imaging light and an image side facing the image side and passing the imaging light; the first lens has a positive refractive power; The second lens has a negative refractive power; the third lens has a positive refractive power; at least one of the fourth lens and the fifth lens has a positive refractive power; at least one of the object side and the image side of the sixth lens is aspherical and has An inflection point; Wherein, the optical imaging lens has only six lenses having refractive power, the radius of curvature of the object side surface of the fourth lens is R7, the radius of curvature of the image side surface of the fourth lens is R8, and the radius of curvature of the image side surface of the fifth lens R10, the radius of curvature of the object side of the sixth lens is R11, and satisfies -14.97<R7/R8<-0.12, 0.96<R10/R11<1.41. The optical imaging lens according to claim 19, wherein the object side surface of the second lens is a concave surface, and the image side surface of the second lens is a concave surface. The optical imaging lens according to claim 19, wherein the object side surface of the third lens is a concave surface, and the image side surface of the third lens is a convex surface. The optical imaging lens according to claim 19, wherein the object side surface of the third lens is a convex surface, and the image side surface of the third lens is a concave surface. The optical imaging lens according to claim 19, wherein the object side surface of the fifth lens is a concave surface, and the image side surface of the fifth lens is a convex surface.