TWI802148B

Imaging lens

Abstract

An image lens including five to nine lens elements having refracting power is provided. A first lens element, a second lens element, a third lens element and a fourth lens element are arranged in sequence from a magnified side to a minified side of the image lens. The first and third lens elements are glass lenses. The ratio of the thickness and the diameter of the first lens element is larger than 0.04. At least one of the two lens elements mostly close to the minified side is aspheric. The minimal aperture (aperture diaphragm) of the image lens is disposed between the second lens element and the fourth lens element. The included angle between the chief ray of the image lens and the normal line of the image plane is smaller than 5°. The image lens meets the conditions FOV＜90°, Fno≦1.6 and 0.2＜EFL/LT＜0.35, wherein FOV is the field of view, Fno is the f number, EFL is the effective focal length, and LT is the distance between the outer surfaces of the two most outlying lens elements. The modulation transfer function of the image lens is higher than 30% for the wavelength of 940 nm and the spatial frequency of 40 lp/mm.

TWI802148B, drawing sheet 1 — Sheet 1 of 13

Term

No projected expiry on record.

12 claims: 12 independent, 0 dependent

1
An imaging lens, comprising:5 to 9 lenses with diopters, a first lens, a second lens, a third lens and a fourth lens are arranged in sequence from an enlargement side to a reduction side of the imaging lens, The first lens and the third lens are glass lenses, the ratio of the thickness to the diameter of the first lens is greater than 0.04, and at least one of the two lenses closest to the reduction side is an aspheric mirror, wherein the minimum lens of the imaging lens The optical aperture is arranged between the second lens and the fourth lens, the angle between the chief ray of the imaging lens and the normal of an imaging surface is less than 5, and the imaging lens satisfies the conditional formula FOV<90°, Fno1.6, 0.2 <EFL/LT<0.35, FOV is the full field of view, Fno is the aperture value, EFL is the effective focal length, and LT is the distance between the outer surfaces of the two outermost lenses of the imaging lens, for a wavelength of 940nm and a spatial frequency of 40 lp/mm (line logarithm/mm) light, the modulation transfer function of the imaging lens is greater than 30%. 一種成像鏡頭，包括：5到9片具有屈光度的透鏡，自該成像鏡頭的一放大側至一縮小側依序排列有一第一透鏡、一第二透鏡、一第三透鏡以及一第四透鏡，該第一透鏡及該第三透鏡是玻璃透鏡，該第一透鏡的厚度與直徑的比值大於0.04，最靠近該縮小側的兩片透鏡中的至少一者是非球面鏡，其中該成像鏡頭的最小透光孔徑設置於該第二透鏡以及該第四透鏡之間，該成像鏡頭的主光線與一成像面的法線的夾角小於5，該成像鏡頭滿足條件式FOV<90°，Fno≦1.6，0.2<EFL/LT<0.35，FOV為全視場角，Fno為光圈值，EFL為有效焦距，且LT為該成像鏡頭最外側兩片透鏡的外表面的距離，對於波長為940nm且空間頻率為40 lp/mm(線對數/毫米)的光，該成像鏡頭的調製傳遞函數大於30%。
2
The imaging lens as described in claim 1, the imaging lens at least meets one of the following conditions:(1) the thickness of the first lens is greater than 0.95 mm;(2) the total length from the first lens to the imaging surface is less than 60 mm;(3) The F-theta distortion of the imaging lens is less than 1.5%;(4) The imaging lens includes a glass-plastic hybrid lens;(5) The cone angle of each field of view is greater than 30 degrees. 如請求項1所述的成像鏡頭，該成像鏡頭至少滿足下列條件之一：(1)該第一透鏡的厚度大於0.95mm；(2)該第一透鏡到該成像面的總長度小於60mm；(3)該成像鏡頭的F-theta畸變小於1.5%；(4)該成像鏡頭包括玻塑混合透鏡；(5)各視場的圓錐角大於30度。
3
As for the imaging lens described in claim 1, the positive and negative values of the diopters of the lenses arranged sequentially from the magnifying side to the reducing side of the imaging lens meet at least one of the following conditions:(1) negative positive positive positive positive;(2) (3) Negative Positive Positive Positive Positive;(4) Negative Positive Positive Negative Negative Positive;(5) Negative Positive Positive Negative Negative Positive;(6) Positive Negative Positive Positive Negative Positive Positive. 如請求項1所述的成像鏡頭，該成像鏡頭自該放大側至該縮小側依序排列的透鏡的屈光度的正負值至少滿足下列條件之一：(1)負正正正正；(2)負正正負負正；(3)負負正正正正；(4)負負正負負正正；(5)負負正正負負正正；(6)正負正正負正正正。
4
The imaging lens as described in claim 1, the imaging lens at least meets one of the following conditions:(1) 13.8mm<EFL<14.5mm;(2) 0.15<LT/ImgH<0.19, where ImgH is the maximum image height (3 )8.0mm<ImgH<8.5mm;(4) The ratio of the diameter of the lens closest to the enlargement side to the diameter of the lens closest to the reduction side falls within the range of 0.8 to 1.35. 如請求項1所述的成像鏡頭，該成像鏡頭至少滿足下列條件之一：(1)13.8mm<EFL<14.5mm；(2)0.15<LT/ImgH<0.19，其中ImgH為最大像高(3)8.0mm<ImgH<8.5mm；(4)最靠近該放大側的透鏡的直徑以及最靠近該縮小側的透鏡的直徑的比值落在0.8至1.35的範圍內。
5
The imaging lens as described in Claim 1, the imaging lens at least meets one of the following conditions:(1) FOV<70°;(2) includes at least one piece of glass molded lens;(3) has no cemented lens;(4) includes at least A cemented lens, and the distance between the at least one cemented lens is less than 0.01 mm. 如請求項1所述的成像鏡頭，該成像鏡頭至少滿足下列條件之一：(1)FOV<70°；(2)包括至少一片玻璃模造透鏡；(3)無膠合透鏡；(4)包括至少一膠合透鏡，且該至少一膠合透鏡的間隔小於0.01mm。
6
As for the imaging lens described in claim 1, the lenses arranged sequentially from the magnification side to the reduction side of the imaging lens at least meet one of the following conditions:(1) biconcave, aspheric, biconvex, aspheric and aspheric Lenses;(2) biconcave, aspheric, biconvex, aspheric, aspheric and aspheric lenses;(3) plano-concave, aspheric, biconvex, aspheric, aspheric and aspheric lenses;(4) new Lunar, aspheric, biconvex, aspheric, crescent, aspheric, and aspheric lenses;(5) Crescent, biconcave, biconvex, biconvex, crescent, crescent, aspheric, and crescent lenses;( 6) Crescent, crescent, bi-convex, crescent, bi-concave, crescent, bi-convex, and crescent lenses. 如請求項1所述的成像鏡頭，該成像鏡頭自該放大側至該縮小側依序排列的透鏡至少滿足下列條件之一：(1)雙凹、非球面、雙凸、非球面和非球面透鏡；(2)雙凹、非球面、雙凸、非球面、非球面和非球面透鏡；(3)平凹、非球面、雙凸、非球面、非球面和非球面透鏡；(4)新月、非球面、雙凸、非球面、新月、非球面和非球面透鏡；(5)新月、雙凹、雙凸、雙凸、新月、新月、非球面和新月透鏡；(6)新月、新月、雙凸、新月、雙凹、新月、雙凸和新月透鏡。
7
An imaging lens, comprising:7 to 9 lenses with diopters, and these lenses are all glass lenses, the ratio of the thickness to the diameter of a first lens closest to the magnification side of the imaging lens is greater than 0.04, wherein the imaging lens The included angle between the chief ray and the normal of an imaging surface is less than 5°, the imaging lens satisfies the conditions of FOV<90°, Fno1.6, 0.2<EFL/LT<0.35, FOV is the full field of view, Fno is the aperture value, EFL is the effective focal length, and LT is the distance between the outer surfaces of the two outermost lenses of the lens. For light with a wavelength of 940nm and a spatial frequency of 40 lp/mm (line logarithm/mm), the modulation transfer function of the imaging lens is greater than 30 %. 一種成像鏡頭，包括：7到9片具有屈光度的透鏡，且該些透鏡皆為玻璃透鏡，最靠近該成像鏡頭放大側的一第一透鏡的厚度與直徑的比值大於0.04，其中該成像鏡頭的主光線與一成像面的法線的夾角小於5°，該成像鏡頭滿足條件式FOV<90°，Fno≦1.6，0.2<EFL/LT<0.35，FOV為全視場角，Fno為光圈值，EFL為有效焦距，且LT為鏡頭最外側兩片透鏡的外表面的距離，對於波長為940nm且空間頻率為40 lp/mm(線對數/毫米)的光，該成像鏡頭的調製傳遞函數大於30%。
8
The imaging lens as described in Claim 7, the imaging lens at least meets one of the following conditions:(1) the thickness of the first lens is greater than 0.95 mm;(2) the total length from the first lens to the imaging surface is less than 60 mm;(3) The F-theta distortion of the imaging lens is less than 1.5%;(4) the cone angle of each field of view is greater than 30 degrees. 如請求項7所述的成像鏡頭，該成像鏡頭至少滿足下列條件之一：(1)該第一透鏡的厚度大於0.95mm；(2)該第一透鏡到該成像面的總長度小於60mm；(3)該成像鏡頭的F-theta畸變小於1.5%；(4)各視場的圓錐角大於30度。
9
As for the imaging lens described in claim 7, the positive and negative values of the diopters of the lenses arranged sequentially from the magnifying side to the reducing side of the imaging lens meet at least one of the following conditions:(1) negative negative positive negative positive negative negative positive positive;2) Positive negative positive positive negative positive positive positive. 如請求項7所述的成像鏡頭，該成像鏡頭自該放大側至該縮小側依序排列的透鏡的屈光度的正負值至少滿足下列條件之一：(1)負負正正負負正正；(2)正負正正負正正正。
10
The imaging lens as described in claim item 7, the imaging lens at least meets one of the following conditions:(1) 13.8mm<EFL<14.5mm;(2) 0.15<LT/ImgH<0.19, where ImgH is the maximum image height (3 )8.0mm<ImgH<8.5mm;(4) The ratio of the diameter of the lens closest to the enlargement side to the diameter of the lens closest to the reduction side falls within the range of 0.8 to 1.35. 如請求項7所述的成像鏡頭，該成像鏡頭至少滿足下列條件之一：(1)13.8mm<EFL<14.5mm；(2)0.15<LT/ImgH<0.19，其中ImgH為最大像高(3)8.0mm<ImgH<8.5mm；(4)最靠近該放大側的透鏡的直徑以及最靠近該縮小側的透鏡的直徑的比值落在0.8至1.35的範圍內。
11
The imaging lens as described in Claim 7, the imaging lens at least meets one of the following conditions:(1) FOV<70°;(2) includes at least one piece of glass molded lens;(3) has no cemented lens;(4) includes at least A cemented lens, and the distance between the at least one cemented lens is less than 0.01 mm. 如請求項7所述的成像鏡頭，該成像鏡頭至少滿足下列條件之一：(1)FOV<70°；(2)包括至少一片玻璃模造透鏡；(3)無膠合透鏡；(4)包括至少一膠合透鏡，且該至少一膠合透鏡的間隔小於0.01mm。
12
As for the imaging lens described in claim 7, the lenses arranged sequentially from the magnification side to the reduction side of the imaging lens at least meet one of the following conditions:(1) Crescent, biconcave, biconvex, biconvex, crescent , crescent, aspheric and crescent lenses;(2) crescent, crescent, biconvex, crescent, biconcave, crescent, biconvex and crescent lenses. 如請求項7所述的成像鏡頭，該成像鏡頭自該放大側至該縮小側依序排列的透鏡至少滿足下列條件之一：(1)新月、雙凹、雙凸、雙凸、新月、新月、非球面和新月透鏡；(2)新月、新月、雙凸、新月、雙凹、新月、雙凸和新月透鏡。

Independent claims12

82 paragraphs in 1 section, as filed

imaging lens

IMAGING LENS

The invention relates to an optical element, especially an imaging lens.

In recent years, imaging lenses have continued to evolve. It has always been a development goal of imaging lens design to provide an imaging lens that is thin, light, small and has good imaging quality. In addition, small f-stops can increase the amount of light passing through, and large image heights can increase the pixel size.

In addition to requiring a small aperture value, it is also necessary to consider the cost and temperature resistance of the lens material. Using glass as the material of the lens has a problem of high cost. Plastic lenses have the problem of not being able to withstand high temperatures. In view of this, how to design an imaging lens with large image height, small aperture value, low cost and high temperature resistance is also the focus of research and development under the premise of pursuing light, thin and small lenses.

The invention provides an imaging lens with large image height, small aperture value, small aberration, high temperature resistance and low cost.

According to an embodiment of the present invention, an imaging lens is provided, including 5 to 9 lenses with diopters, and a first lens, a second lens, a third lens and a fourth lens are arranged in sequence from the enlargement side to the reduction side of the imaging lens , the first lens and the third lens are glass lenses, the ratio of the thickness to diameter of the first lens is greater than 0.04, and at least one of the two lenses closest to the reduction side is an aspheric mirror, wherein the minimum light transmission aperture (aperture) of the imaging lens ) is arranged between the second lens and the fourth lens, the angle between the chief ray of the imaging lens and the normal line of the imaging surface is less than 5°, and the imaging lens satisfies the conditions of FOV<90°, Fno1.6, 0.2<EFL/LT< 0.35, FOV is the full field of view, Fno is the aperture value, EFL is the effective focal length, and LT is the distance between the outer surfaces of the two outermost lenses of the lens, for a wavelength of 940 nm and a spatial frequency of 40 lp/mm (line logarithm / mm) light, the modulation transfer function of the imaging lens is greater than 30%.

According to an embodiment of the present invention, an imaging lens is provided, including 7 to 9 lenses with diopters, and these lenses are all glass lenses, and the ratio of the thickness to the diameter of the first lens closest to the magnification side of the imaging lens is greater than 0.04, The angle between the chief ray of the imaging lens and the normal of the imaging surface is less than 5°, and the imaging lens satisfies the conditions of FOV<90°, Fno1.6, 0.2<EFL/LT<0.35, FOV is the full field of view, and Fno is the aperture value, EFL is the effective focal length, and LT is the distance between the outer surfaces of the two outermost lenses of the lens, for light with a wavelength of 940 nm and a spatial frequency of 40 lp/mm (line logarithm/mm), the modulation transfer function of the imaging lens Greater than 30%.

Based on the above, the imaging lens provided by the embodiment of the present invention satisfies the condition Fno1.6 and has a large aperture. It also includes a glass lens for high temperature resistance. And the aberration of the imaging lens is small.

In order to make the above-mentioned features and advantages of the present invention more comprehensible, the following specific embodiments are described in detail together with the accompanying drawings.

FIG. 1 is a schematic diagram of the imaging lens of the first embodiment of the present invention, and FIGS. 2A to 2D are diagrams of longitudinal spherical aberration and various aberrations of the imaging lens of the first embodiment. Please refer to FIG. 1 first. The imaging lens 1000 of the first embodiment of the present invention includes a first lens 1, a second lens 2, and a third lens along an optical axis I of the imaging lens 1000 from the object side A1 to the image side A2. 3. Aperture 0, fourth lens 4, fifth lens 5, optical filter 9 and cover glass 10, wherein the first lens 1 and the third lens 3 are glass lenses, the second lens 2, the fourth lens 4 and the second lens The five lenses 5 are plastic lenses. When the light emitted by an object to be photographed enters the imaging lens 1000, and passes through the first lens 1, the second lens 2, the third lens 3, the aperture 0, the fourth lens 4, the fifth lens 5, the filter 9 and the cover glass 10, an image will be formed on the imaging surface 100 (image plane). The filter 9 is, for example, an infrared pass filter (infrared pass filter), which can allow light with an appropriate wavelength to pass through while filtering out a desired waveband. The filter 9 is disposed between the fifth lens 5 and the cover glass 10 . It is supplemented that the object side A1 is the side facing the object to be photographed, also referred to as the magnification side. The image side A2 is the side facing the imaging surface 100 , also referred to as the reduction side.

In this embodiment, the first lens 1, the second lens 2, the third lens 3, the fourth lens 4, the fifth lens 5, the filter 9 and the cover glass 10 of the imaging lens 1000 each have And the object side 15, 25, 35, 45, 55, 95, 105 through which the imaging light passes and the image side 16, 26, 36, 46, 56, 96, 106 facing the image side A2 through which the imaging light passes. In this embodiment, the aperture 0 is disposed between the third lens 3 and the fourth lens 4 , and the aperture 0 is also the minimum light transmission aperture of the lens barrel.

The first lens 1 has negative refracting power. Both the object side 15 and the image side 16 of the first lens 1 are spherical surfaces. The second lens 2 has a positive refractive power. Both the object side 25 and the image side 26 of the second lens 2 are aspheric surfaces. The third lens 3 has positive refractive power. Both the object side 35 and the image side 36 of the third lens 3 are spherical. The fourth lens 4 has positive refractive power. Both the object side 45 and the image side 46 of the fourth lens 4 are aspherical. The fifth lens 5 has positive refractive power. Both the object side 55 and the image side 56 of the fifth lens 5 are aspherical.

Other detailed optical data of the first embodiment are shown in Table 1 below, and the effective focal length (Effective Focal Length, EFL) of the imaging lens 1000 of the first embodiment is 14.3 mm (millimeter, mm), and the full field of view (field of view, FOV) is 67°, the total length of the lens is 55 mm, and the aperture value (F-number, Fno) is 1.47, the maximum image height is 8.3 mm, and the total length of the lens unit is 46.9 mm, where the total length of the lens refers to the distance from the object side 15 of the first lens 1 to the imaging surface 100 on the optical axis I, and the total length of the lens unit refers to the distance on the optical axis I from the object side 15 of the first lens 1 to the image side 56 of the fifth lens 5 . It should be noted that the radius of curvature of the object side 15 shown in Table 1 refers to the radius of curvature of the object side 15 of the first lens 1 in the optical axis region, and the radius of curvature of the image side 16 refers to the image of the first lens 1. The radius of curvature of the side surface 16 in the region of the optical axis, and so on. The distance between the object side 15 (as shown in Table 1 is 1.11 mm) refers to the distance between the object side 15 and the next surface (the image side 16 in this example) on the optical axis I, that is, the first lens 1 on the optical axis The thickness on I is 1.11 mm, and the distance between the image side 16 (as shown in Table 1 is 7.09 mm) refers to the distance between the image side 16 and the object side 25 on the optical axis I, that is, the first lens 1 and the second lens 2 The gap on the optical axis I is 7.09 mm, and so on.

Table I: <tables><table><table border="1" borderColor="#000000" width="85%"><tbody><tr><td>first embodiment </td></tr><tr><td>Effective focal length = 14.3 mm, full field of view = 67°, total lens length = 55 mm, aperture value = 1.47, Large image height = 8.3 mm, total lens length = 46.9 mm </td></tr><tr><td>element </td><td>noodle </td><td>Radius of curvature (mm) </td><td>spacing mm) </td><td>Refractive index </td><td>Abbe number </td></tr><tr><td>object </td><td> </td><td>Unlimited </td><td>Unlimited </td><td> </td><td> </td></tr><tr><td>first lens 1 </td><td>object side 15 </td><td>-59.19 </td><td>1.11 </td><td>1.52 </td><td>64 </td></tr><tr><td> </td><td>like side 16 </td><td>14.32 </td><td>7.09 </td><td> </td><td> </td></tr><tr><td>second lens 2 </td><td>object side 25 </td><td>-29.16 </td><td>5.11 </td><td>1.64 </td><td>twenty four </td></tr><tr><td> </td><td>like profile 26 </td><td>-22.70 </td><td>0.20 </td><td> </td><td> </td></tr><tr><td>third lens 3 </td><td>object side 35 </td><td>19.24 </td><td>4.80 </td><td>1.88 </td><td>41 </td></tr><tr><td> </td><td>like side 36 </td><td>-139.18 </td><td>4.06 </td><td> </td><td> </td></tr><tr><td>Aperture 0 </td><td> </td><td>Unlimited </td><td>8.13 </td><td> </td><td> </td></tr><tr><td>Fourth lens 4 </td><td>object side 45 </td><td>-8.65 </td><td>8.50 </td><td>1.64 </td><td>twenty four </td></tr><tr><td> </td><td>like side 46 </td><td>-10.17 </td><td>0.10 </td><td> </td><td> </td></tr><tr><td>fifth lens 5 </td><td>object side 55 </td><td>16.50 </td><td>7.77 </td><td>1.64 </td><td>twenty four </td></tr><tr><td> </td><td>like profile 56 </td><td>41.86 </td><td>4.18 </td><td> </td><td> </td></tr><tr><td>Filter 9 </td><td>object side 95 </td><td>Unlimited </td><td>0.40 </td><td>1.52 </td><td>64 </td></tr><tr><td> </td><td>like profile 96 </td><td>Unlimited </td><td>3.00 </td><td> </td><td> </td></tr><tr><td>cover glass 10 </td><td>object side 105 </td><td>Unlimited </td><td>0.50 </td><td>1.52 </td><td>64 </td></tr><tr><td> </td><td>like profile 106 </td><td>Unlimited </td><td>0.05 </td><td> </td><td> </td></tr><tr><td> </td><td>Imaging surface 100 </td><td>Unlimited </td><td>0.00 </td><td> </td><td> </td></tr></tbody></table></table></tables>

According to Table 1, the first lens 1 is a biconcave lens, the object side 15 is concave, and the image side 16 is concave. The second lens 2 is an aspherical lens with a convex surface facing the image side A2, the object side surface 25 is concave, and the image side surface 26 is convex. The third lens 3 is a biconvex lens, the object side 35 is convex, and the image side 36 is convex. The fourth lens 4 is an aspherical lens with a convex surface facing the image side A2, the object side surface 45 is concave, and the image side 46 is convex. The fifth lens 5 is an aspherical lens with a convex surface facing the object side A1, the object side 55 is convex, and the image side 56 is concave.

In this embodiment, the ratio of the thickness to the diameter of the first lens 1 is greater than 0.035, preferably greater than 0.04, the thickness refers to the thickness of the optical center of the first lens 1, that is, the thickness on the optical axis I, and the diameter refers to the thickness of the first lens. 1 The distance between the turning points on both sides of the optical center, that is, the distance between point P and point Q in Figure 1, for example, the diameter of the object side 15 of the first lens 1 is the curved surface of the object side 15 from the optical center The distance between the two places where the edge of the side lens extends and turns. Taking this embodiment as an example, the first lens has a thickness of 1.11 mm and a diameter of 26.10 mm. The included angle between the chief ray of the imaging lens 1000 and the normal of the imaging surface 100 is less than 5°. The maximum image height is 8.3 mm. The cone angle of each field of view is greater than 30 degrees. For light with a wavelength of 940 nm and a spatial frequency of 40 lp/mm (line log/mm), the modulation transfer function of the imaging lens 1000 is greater than 30%.

In addition, in this embodiment, the object side 25, 45, 55 and image side 26, 46, 56 of the second lens 2, the fourth lens 4, and the fifth lens 5 have a total of six aspherical surfaces, and these aspherical surfaces is defined according to the following formula: <img file="TWI802148B_D0001.tif" />...(1) : the distance between the point on the aspheric curve and the optical axis; : Depth of the aspheric surface, that is, the vertical distance between the point on the aspheric surface whose distance from the optical axis is Y, and the tangent plane tangent to the vertex on the aspheric surfaces optical axis; : radius of curvature of the lens surface; : cone coefficient; 2i: 2ith-order aspheric coefficient.

Each of the above-mentioned aspherical second lens 2, fourth lens 4 and fifth lens 5 can be replaced by two spherical lenses, and the number of lens sheets of the lens is between 5 and 8, so as to avoid the possible problem of higher costs. The various aspheric coefficients of the above-mentioned aspheric surface in formula (1) are shown in Table 2 below. Wherein, the column number 25 in Table 2 indicates that it is the aspheric coefficient of the object side surface 25 of the second lens 2 , and other columns can be deduced by analogy. In this embodiment, the twelfth-order aspheric coefficient a of the above-mentioned aspheric surface 12and the 14th order aspheric coefficient a 14are all zero.

Table II: <tables><table><table border="1" borderColor="#000000" width="85%"><tbody><tr><td>noodle </td><td>R </td><td>K </td><td>a 4 </td><td>a 6 </td></tr><tr><td>25 </td><td>-29.15882296 </td><td>-0.886909116 </td><td>-2.94619E-05 </td><td>-1.73218E-07 </td></tr><tr><td>26 </td><td>-22.7042 </td><td>-1.16826 </td><td>-2.9E-05 </td><td>-9.8E-08 </td></tr><tr><td>45 </td><td>-8.64894 </td><td>-0.504626 </td><td>-5.12E-05 </td><td>1.93E-07 </td></tr><tr><td>46 </td><td>-10.1677 </td><td>-1.04882 </td><td>3.88E-05 </td><td>-4.3E-07 </td></tr><tr><td>55 </td><td>16.501213 </td><td>-0.775734 </td><td>2.584E-05 </td><td>-1.73E-07 </td></tr><tr><td>56 </td><td>41.85627 </td><td>-59.6228 </td><td>-8.6E-05 </td><td>5.62E-07 </td></tr><tr><td>noodle </td><td>a 8 </td><td>a 10 </td><td>a 12 </td><td>a 14 </td></tr><tr><td>25 </td><td>0.00E+00 </td><td>0.00E+00 </td><td>0.00E+00 </td><td>0.00E+00 </td></tr><tr><td>26 </td><td>0.00E+00 </td><td>0.00E+00 </td><td>0.00E+00 </td><td>0.00E+00 </td></tr><tr><td>45 </td><td>2.86E-08 </td><td>-1.82E-10 </td><td>0.00E+00 </td><td>0.00E+00 </td></tr><tr><td>46 </td><td>6.8E-09 </td><td>-6.8E-12 </td><td>0.00E+00 </td><td>0.00E+00 </td></tr><tr><td>55 </td><td>2.03E-09 </td><td>-7.44E-12 </td><td>0.00E+00 </td><td>0.00E+00 </td></tr><tr><td>56 </td><td>-1.3E-09 </td><td>-2.9E-12 </td><td>0.00E+00 </td><td>0.00E+00 </td></tr></tbody></table></table></tables>

Referring to Fig. 2A to Fig. 2D again, Fig. 2A illustrates the longitudinal spherical aberration (Longitudinal Spherical Aberration) of the first embodiment, and Fig. 2B and Fig. 2C respectively illustrate the first embodiment when the wavelength is 960 nm and 940 nm and field curvature aberration in the sagittal direction and field curvature aberration in the meridional direction on the imaging plane 100 at 920 nm, the diagram in FIG. 2D illustrates the first embodiment when its Distortion Aberration on the imaging surface 100 at wavelengths of 960 nm, 940 nm and 920 nm. In Fig. 2A of the longitudinal spherical aberration diagram of the first embodiment, it can be seen from the deflection amplitude of each curve representing the wavelength that the imaging point deviation of off-axis rays at different heights is controlled within ±0.05 millimeters (mm) range, so the first embodiment does significantly improve spherical aberration at the same wavelength. In addition, the distances between the three representative wavelengths are quite close to each other, and the imaging positions representing different wavelengths of light are quite concentrated, so that the chromatic aberration is also significantly improved.

In the two field curvature aberration diagrams of Fig. 2B and Fig. 2C, the field curvature aberrations of the three representative wavelengths in the entire field of view fall within ±0.08 mm, indicating that the optical system of the first embodiment can effectively eliminate aberrations. The distortion aberration diagram in FIG. 2D shows that the distortion aberration of the first embodiment is maintained within the range of ±13%, indicating that the distortion aberration of the first embodiment meets the imaging quality requirements of the optical system. Compared with the existing imaging lens, the first embodiment can still provide good imaging quality under the condition that the total length of the lens is 55 mm, the aperture value is 1.47, the maximum image height is 8.3 mm, and some lenses are made of plastic lenses.

In this embodiment, the F-theta distortion of the imaging lens 1000 is less than ±1.15%. The cone angle (Cone angle) of each field of view light is larger than 30°. The imaging lens 1000 does not have a cemented lens.

FIG. 3 is a schematic diagram of the imaging lens of the second embodiment of the present invention, and FIGS. 4A to 4D are diagrams of longitudinal spherical aberration and various aberrations of the imaging lens of the second embodiment. Please refer to FIG. 3 first. The imaging lens 1000 of the second embodiment of the present invention includes a first lens 1, a second lens 2, and a third lens along an optical axis I of the imaging lens 1000 from the object side A1 to the image side A2. 3. Aperture 0, fourth lens 4, fifth lens 5, sixth lens 6, optical filter 9 and cover glass 10, wherein the first lens 1 and the third lens 3 are glass lenses, the second lens 2, the second lens The four lenses 4, the fifth lens 5 and the sixth lens 6 are plastic lenses. When the light emitted by an object to be photographed enters the imaging lens 1000, and passes through the first lens 1, the second lens 2, the third lens 3, the aperture 0, the fourth lens 4, the fifth lens 5, and the sixth lens 6. After the filter 9 and the cover glass 10 , an image will be formed on the imaging surface 100 . The filter 9 is, for example, an infrared pass filter. The filter 9 is disposed between the sixth lens 6 and the cover glass 10 .

In this embodiment, the first lens 1, the second lens 2, the third lens 3, the fourth lens 4, the fifth lens 5, the sixth lens 6, the filter 9 and the cover glass 10 of the imaging lens 1000 are each There are object sides 15, 25, 35, 45, 55, 65, 95, 105 facing the object side A1 and allowing the imaging rays to pass therethrough, and image sides 16, 26, 36, 46, 56 facing the image side A2 and allowing the imaging rays to pass therethrough , 66, 96, 106. In this embodiment, the aperture 0 is disposed between the third lens 3 and the fourth lens 4 .

The first lens 1 has a negative refractive power. Both the object side 15 and the image side 16 of the first lens 1 are spherical. The second lens 2 has a positive refractive power. Both the object side 25 and the image side 26 of the second lens 2 are aspherical. The third lens 3 has positive refractive power. Both the object side 35 and the image side 36 of the third lens 3 are spherical. The fourth lens 4 has a negative refractive power. Both the object side 45 and the image side 46 of the fourth lens 4 are aspherical. The fifth lens 5 has negative refractive power. Both the object side 55 and the image side 56 of the fifth lens 5 are aspherical. The sixth lens 6 has positive refractive power. Both the object side 65 and the image side 66 of the sixth lens 6 are aspherical.

Other detailed optical data of the second embodiment are shown in Table 3 below.

Table three: <tables><table><table border="1" borderColor="#000000" width="85%"><tbody><tr><td>second embodiment </td></tr><tr><td>Effective focal length = 14.3 mm, full field of view = 68°, total lens length = 55 mm, aperture value = 1.31, Large image height = 8.3 mm, total lens length = 47.2 mm </td></tr><tr><td>element </td><td>noodle </td><td>Radius of curvature (mm) </td><td>spacing mm) </td><td>Refractive index </td><td>Abbe number </td></tr><tr><td>object </td><td> </td><td>Unlimited </td><td>Unlimited </td><td> </td><td> </td></tr><tr><td>first lens 1 </td><td>object side 15 </td><td>-37.46 </td><td>0.99 </td><td>1.52 </td><td>64 </td></tr><tr><td> </td><td>like side 16 </td><td>15.67 </td><td>5.53 </td><td> </td><td> </td></tr><tr><td>second lens 2 </td><td>object side 25 </td><td>-40.38 </td><td>8.53 </td><td>1.64 </td><td>twenty four </td></tr><tr><td> </td><td>like profile 26 </td><td>-23.26 </td><td>0.44 </td><td> </td><td> </td></tr><tr><td>third lens 3 </td><td>object side 35 </td><td>30.64 </td><td>4.30 </td><td>1.88 </td><td>41 </td></tr><tr><td> </td><td>like side 36 </td><td>-43.88 </td><td>1.21 </td><td> </td><td> </td></tr><tr><td>Aperture 0 </td><td> </td><td>Unlimited </td><td>0.10 </td><td> </td><td> </td></tr><tr><td>Fourth lens 4 </td><td>object side 45 </td><td>13.91 </td><td>3.00 </td><td>1.64 </td><td>twenty four </td></tr><tr><td> </td><td>like side 46 </td><td>10.74 </td><td>10.00 </td><td> </td><td> </td></tr><tr><td>fifth lens 5 </td><td>object side 55 </td><td>-5.34 </td><td>3.00 </td><td>1.64 </td><td>twenty four </td></tr><tr><td> </td><td>like profile 56 </td><td>-9.14 </td><td>0.10 </td><td> </td><td> </td></tr><tr><td>sixth lens 6 </td><td>object side 65 </td><td>12.08 </td><td>10.00 </td><td>1.64 </td><td>twenty four </td></tr><tr><td> </td><td>like side 66 </td><td>-30.26 </td><td>3.86 </td><td> </td><td> </td></tr><tr><td>Filter 9 </td><td>object side 95 </td><td>Unlimited </td><td>0.40 </td><td>1.52 </td><td>64 </td></tr><tr><td> </td><td>like profile 96 </td><td>Unlimited </td><td>3.00 </td><td> </td><td> </td></tr><tr><td>cover glass 10 </td><td>object side 105 </td><td>Unlimited </td><td>0.50 </td><td>1.52 </td><td>64 </td></tr><tr><td> </td><td>like profile 106 </td><td>Unlimited </td><td>0.05 </td><td> </td><td> </td></tr><tr><td> </td><td>Imaging surface 100 </td><td>Unlimited </td><td>0.00 </td><td> </td><td> </td></tr></tbody></table></table></tables>

According to Table 3, the first lens 1 is a biconcave lens, the object side 15 is concave, and the image side 16 is concave. The second lens 2 is an aspherical lens with a convex surface facing the image side A2, the object side surface 25 is concave, and the image side surface 26 is convex. The third lens 3 is a biconvex lens, the object side 35 is convex, and the image side 36 is convex. The fourth lens 4 is an aspheric lens with a convex surface facing the object side A1, the object side 45 is convex, and the image side 46 is concave. The fifth lens 5 is an aspherical lens with a convex surface facing the image side A2, the object side surface 55 is concave, and the image side 56 is convex. The sixth lens 6 is an aspherical lens with a convex object side 65 and a convex image side 66 .

The ratio of the thickness to the diameter of the first lens 1 is greater than 0.035, preferably greater than 0.04. Taking this embodiment as an example, the thickness refers to the thickness of the optical center of the first lens 1 on the optical axis I, and the diameter refers to the optical center of the first lens 1. The distance between the turning points on both sides of the center, the thickness of the first lens is 0.99 mm, and the diameter is 23.54 mm. In addition, in this embodiment, the second lens 2, the fourth lens 4, the fifth lens 5, and the sixth lens 6 have eight object sides 25, 45, 55, 65 and image sides 26, 46, 56, 66 in total. The surfaces are all aspherical surfaces, and these aspheric surfaces are defined according to the above formula (1).

Three of the above-mentioned aspherical second lens 2, fourth lens 4, fifth lens 5, and sixth lens 6 can be selected, each of which can be replaced by two spherical lenses, so that the number of lenses in the lens is between 6 to 9 elements to avoid the problem of higher cost that may be caused by aspheric lenses. The various aspheric coefficients of the above-mentioned aspheric surface in the formula (1) are shown in Table 4 and Figure 8 below. Wherein, the column number 25 in Table 4 indicates that it is the aspheric coefficient of the object side surface 25 of the second lens 2 , and the other columns can be deduced by analogy. In this embodiment, the twelfth-order aspheric coefficient a of the above-mentioned aspheric surface 12and the 14th order aspheric coefficient a 14are all zero.

Table four: <tables><table><table border="1" borderColor="#000000" width="85%"><tbody><tr><td>noodle </td><td>R </td><td>K </td><td>a 4 </td><td>a 6 </td></tr><tr><td>25 </td><td>-40.38 </td><td>12.31 </td><td>-4.69E-05 </td><td>-1.44E-07 </td></tr><tr><td>26 </td><td>-23.26 </td><td>-4.52 </td><td>-6.01E-05 </td><td>-3.23E-09 </td></tr><tr><td>45 </td><td>13.91 </td><td>0.00E+00 </td><td>2.20E-06 </td><td>0.00E+00 </td></tr><tr><td>46 </td><td>10.74 </td><td>0.00E+00 </td><td>-1.93E-05 </td><td>0.00E+00 </td></tr><tr><td>55 </td><td>-5.34 </td><td>-2.70 </td><td>-2.96E-04 </td><td>7.87E-06 </td></tr><tr><td>56 </td><td>-9.14 </td><td>-4.17 </td><td>-1.33E-04 </td><td>4.95E-06 </td></tr><tr><td>65 </td><td>12.08 </td><td>-6.92 </td><td>1.36E-04 </td><td>-4.74E-07 </td></tr><tr><td>66 </td><td>-30.26 </td><td>0.00E+00 </td><td>1.47E-05 </td><td>8.60E-07 </td></tr><tr><td>noodle </td><td>a 8 </td><td>a 10 </td><td>a 12 </td><td>a 14 </td></tr><tr><td>25 </td><td>0.00E+00 </td><td>0.00E+00 </td><td>0.00E+00 </td><td>0.00E+00 </td></tr><tr><td>26 </td><td>0.00E+00 </td><td>0.00E+00 </td><td>0.00E+00 </td><td>0.00E+00 </td></tr><tr><td>45 </td><td>0.00E+00 </td><td>0.00E+00 </td><td>0.00E+00 </td><td>0.00E+00 </td></tr><tr><td>46 </td><td>0.00E+00 </td><td>0.00E+00 </td><td>0.00E+00 </td><td>0.00E+00 </td></tr><tr><td>55 </td><td>-1.06E-07 </td><td>5.40E-10 </td><td>0.00E+00 </td><td>0.00E+00 </td></tr><tr><td>56 </td><td>-5.41E-08 </td><td>2.10E-10 </td><td>0.00E+00 </td><td>0.00E+00 </td></tr><tr><td>65 </td><td>2.07E-09 </td><td>-3.75E-12 </td><td>0.00E+00 </td><td>0.00E+00 </td></tr><tr><td>66 </td><td>-3.76E-09 </td><td>1.92E-12 </td><td>0.00E+00 </td><td>0.00E+00 </td></tr></tbody></table></table></tables>

Referring to Fig. 4A to Fig. 4D, Fig. 4A illustrates the longitudinal spherical aberration of the second embodiment, and Fig. 4B and Fig. 4C respectively illustrate the second embodiment when the wavelength is 960 nm, 940 nm and 920 nm. The field curvature aberration in the sagittal direction and the field curvature aberration in the meridian direction on the imaging plane 100. The diagram in FIG. Distortion aberrations on . In the longitudinal spherical aberration diagram of the second embodiment shown in FIG. 4A , it can be seen from the deflection amplitude of each curve representing the wavelength that the deviation of the imaging point of off-axis rays at different heights is controlled within the range of ±0.03 millimeters. Therefore, the second embodiment does significantly improve spherical aberration at the same wavelength. In addition, the distances between the three representative wavelengths are quite close to each other, and the imaging positions representing different wavelengths of light are quite concentrated, so that the chromatic aberration is also significantly improved.

In the two field curvature aberration diagrams of Fig. 4B and Fig. 4C, the field curvature aberrations of the three representative wavelengths in the entire field of view fall within ±0.06 mm, indicating that the optical system of the second embodiment can effectively eliminate aberrations. The distortion aberration diagram in FIG. 4D shows that the distortion aberration of the second embodiment is maintained within the range of ±14%, indicating that the distortion aberration of the second embodiment meets the imaging quality requirements of the optical system. Compared with the existing imaging lens, the second embodiment can still provide good imaging quality under the condition that the total length of the lens is 55 mm, the aperture value is 1.31, the maximum image height is 8.3 mm, and some lenses are plastic lenses.

FIG. 5 is a schematic diagram of the imaging lens of the third embodiment of the present invention, and FIGS. 6A to 6D are diagrams of longitudinal spherical aberration and various aberrations of the imaging lens of the third embodiment. Please refer to FIG. 5 first. The imaging lens 1000 of the third embodiment of the present invention includes a first lens 1, a second lens 2, and a third lens along an optical axis I of the imaging lens 1000 from the object side A1 to the image side A2. 3. Aperture 0, fourth lens 4, fifth lens 5, sixth lens 6, optical filter 9 and cover glass 10, wherein the first lens 1 and the third lens 3 are glass lenses, the second lens 2, the second lens The four lenses 4, the fifth lens 5 and the sixth lens 6 are plastic lenses. When the light emitted by an object to be photographed enters the imaging lens 1000, and passes through the first lens 1, the second lens 2, the third lens 3, the aperture 0, the fourth lens 4, the fifth lens 5, and the sixth lens 6. After the filter 9 and the cover glass 10 , an image will be formed on the imaging surface 100 . The filter 9 is, for example, an infrared pass filter. The filter 9 is disposed between the sixth lens 6 and the cover glass 10 .

The first lens 1 has a negative refractive power. Both the object side 15 and the image side 16 of the first lens 1 are spherical. The second lens 2 has a negative refractive power. Both the object side 25 and the image side 26 of the second lens 2 are aspherical. The third lens 3 has positive refractive power. Both the object side 35 and the image side 36 of the third lens 3 are spherical. The fourth lens 4 has positive refractive power. Both the object side 45 and the image side 46 of the fourth lens 4 are aspherical. The fifth lens 5 has positive refractive power. Both the object side 55 and the image side 56 of the fifth lens 5 are aspherical. The sixth lens 6 has positive refractive power. Both the object side 65 and the image side 66 of the sixth lens 6 are aspherical.

Other detailed optical data of the third embodiment are shown in Table 5 below.

Table five: <tables><table><table border="1" borderColor="#000000" width="85%"><tbody><tr><td>third embodiment </td></tr><tr><td>Effective focal length = 14.1 mm, full field of view = 69°, total lens length = 55 mm, aperture value = 1.45, Large image height = 8.5 mm, total lens length = 46.2 mm </td></tr><tr><td>element </td><td>noodle </td><td>Radius of curvature (mm) </td><td>spacing mm) </td><td>Refractive index </td><td>Abbe number </td></tr><tr><td>object </td><td> </td><td>Unlimited </td><td>Unlimited </td><td> </td><td> </td></tr><tr><td>first lens 1 </td><td>object side 15 </td><td>Unlimited </td><td>1.00 </td><td>1.52 </td><td>64 </td></tr><tr><td> </td><td>like side 16 </td><td>12.64 </td><td>6.92 </td><td> </td><td> </td></tr><tr><td>second lens 2 </td><td>object side 25 </td><td>-12.69 </td><td>4.34 </td><td>1.64 </td><td>twenty four </td></tr><tr><td> </td><td>like profile 26 </td><td>-15.02 </td><td>0.20 </td><td> </td><td> </td></tr><tr><td>third lens 3 </td><td>object side 35 </td><td>22.23 </td><td>3.78 </td><td>1.88 </td><td>41 </td></tr><tr><td> </td><td>like side 36 </td><td>-90.00 </td><td>0.93 </td><td> </td><td> </td></tr><tr><td>Aperture 0 </td><td> </td><td>Unlimited </td><td>13.06 </td><td> </td><td> </td></tr><tr><td>Fourth lens 4 </td><td>object side 45 </td><td>-37.59 </td><td>4.08 </td><td>1.64 </td><td>twenty four </td></tr><tr><td> </td><td>like side 46 </td><td>-21.26 </td><td>1.71 </td><td> </td><td> </td></tr><tr><td>fifth lens 5 </td><td>object side 55 </td><td>-11.04 </td><td>5.98 </td><td>1.64 </td><td>twenty four </td></tr><tr><td> </td><td>like profile 56 </td><td>-10.94 </td><td>0.10 </td><td> </td><td> </td></tr><tr><td>sixth lens 6 </td><td>object side 65 </td><td>9.38 </td><td>4.14 </td><td>1.64 </td><td>twenty four </td></tr><tr><td> </td><td>like side 66 </td><td>10.66 </td><td>6.84 </td><td> </td><td> </td></tr><tr><td>Filter 9 </td><td>object side 95 </td><td>Unlimited </td><td>0.40 </td><td>1.52 </td><td>64 </td></tr><tr><td> </td><td>like profile 96 </td><td>Unlimited </td><td>1.00 </td><td> </td><td> </td></tr><tr><td>cover glass 10 </td><td>object side 105 </td><td>Unlimited </td><td>0.50 </td><td>1.52 </td><td>64 </td></tr><tr><td> </td><td>like profile 106 </td><td>Unlimited </td><td>0.05 </td><td> </td><td> </td></tr><tr><td> </td><td>Imaging surface 100 </td><td>Unlimited </td><td>0.00 </td><td> </td><td> </td></tr></tbody></table></table></tables>

According to Table 5, the first lens 1 is a plano-concave lens, the object side 15 is flat, and the image side 16 is concave. The second lens 2 is an aspherical lens with a convex surface facing the image side A2, the object side surface 25 is concave, and the image side surface 26 is convex. The third lens 3 is a biconvex lens, the object side 35 is convex, and the image side 36 is convex. The fourth lens 4 is an aspherical lens with a convex surface facing the image side A2, the object side surface 45 is concave, and the image side 46 is convex. The fifth lens 5 is an aspherical lens with a convex surface facing the image side A2, the object side surface 55 is concave, and the image side 56 is convex. The sixth lens 6 is an aspherical lens, the object side 65 is convex, the optical axis area of the image side 66 is concave, and the circumference area of the image side 66 is convex.

The ratio of the thickness of the first lens 1 to the diameter is greater than 0.035, preferably greater than 0.04, the thickness refers to the thickness of the optical center of the first lens 1 on the optical axis I, and the diameter refers to the turning point between the first lens 1 optical center on both sides Taking this embodiment as an example, the thickness of the first lens is 1.00 mm, and the diameter is 22.53 mm. In addition, in this embodiment, the second lens 2, the fourth lens 4, the fifth lens 5, and the sixth lens 6 have eight object sides 25, 45, 55, 65 and image sides 26, 46, 56, 66 in total. The surfaces are all aspherical surfaces, and these aspheric surfaces are defined according to the above formula (1).

Three of the above-mentioned aspherical second lens 2, fourth lens 4, fifth lens 5, and sixth lens 6 can be selected, each of which can be replaced by two spherical lenses, so that the number of lenses in the lens is between 6 to 9 elements to avoid the problem of higher cost that may be caused by aspheric lenses. The various aspheric coefficients of the above-mentioned aspheric surface in formula (1) are shown in Table 6 and Figure 12 below. Wherein, the column number 25 in Table 6 indicates that it is the aspheric coefficient of the object side surface 25 of the second lens 2 , and the other columns can be deduced by analogy.

Table six: <tables><table><table border="1" borderColor="#000000" width="85%"><tbody><tr><td>noodle </td><td>R </td><td>K </td><td>a 4 </td><td>a 6 </td></tr><tr><td>25 </td><td>-12.69 </td><td>0.08 </td><td>4.11E-06 </td><td>0.00E+00 </td></tr><tr><td>26 </td><td>-15.02 </td><td>-0.03 </td><td>4.58E-07 </td><td>0.00E+00 </td></tr><tr><td>45 </td><td>-37.59 </td><td>0.00E+00 </td><td>-2.60E-04 </td><td>-5.26E-07 </td></tr><tr><td>46 </td><td>-21.26 </td><td>0.00E+00 </td><td>2.71E-05 </td><td>5.91E-07 </td></tr><tr><td>55 </td><td>-11.04 </td><td>-0.03 </td><td>7.22E-04 </td><td>-9.86E-06 </td></tr><tr><td>56 </td><td>-10.94 </td><td>-0.19 </td><td>2.02E-04 </td><td>-2.55E-06 </td></tr><tr><td>65 </td><td>9.38 </td><td>-2.55 </td><td>7.92E-05 </td><td>-9.68E-07 </td></tr><tr><td>66 </td><td>10.66 </td><td>-0.19 </td><td>-3.87E-04 </td><td>6.00E-06 </td></tr><tr><td>noodle </td><td>a 8 </td><td>a 10 </td><td>a 12 </td><td>a 14 </td></tr><tr><td>25 </td><td>0.00E+00 </td><td>0.00E+00 </td><td>0.00E+00 </td><td>0.00E+00 </td></tr><tr><td>26 </td><td>0.00E+00 </td><td>0.00E+00 </td><td>0.00E+00 </td><td>0.00E+00 </td></tr><tr><td>45 </td><td>-2.67E-08 </td><td>3.07E-10 </td><td>-6.06E-13 </td><td>-1.15E-14 </td></tr><tr><td>46 </td><td>-4.61E-08 </td><td>7.68E-10 </td><td>-5.28E-12 </td><td>1.37E-14 </td></tr><tr><td>55 </td><td>1.34E-07 </td><td>-1.20E-09 </td><td>6.60E-12 </td><td>-1.55E-14 </td></tr><tr><td>56 </td><td>3.69E-08 </td><td>-2.91E-10 </td><td>1.27E-12 </td><td>-2.01E-15 </td></tr><tr><td>65 </td><td>-5.81E-09 </td><td>4.05E-10 </td><td>-6.07E-12 </td><td>3.88E-14 </td></tr><tr><td>66 </td><td>-1.82E-07 </td><td>3.31E-09 </td><td>-3.69E-11 </td><td>2.12E-13 </td></tr><tr><td>noodle </td><td>a 16 </td><td> </td></tr><tr><td>25 </td><td>0.00E+00 </td><td> </td></tr><tr><td>26 </td><td>0.00E+00 </td><td> </td></tr><tr><td>45 </td><td>0.00E+00 </td><td> </td></tr><tr><td>46 </td><td>0.00E+00 </td><td> </td></tr><tr><td>55 </td><td>0.00E+00 </td><td> </td></tr><tr><td>56 </td><td>0.00E+00 </td><td> </td></tr><tr><td>65 </td><td>-1.06E-16 </td><td> </td></tr><tr><td>66 </td><td>-4.93E-16 </td><td> </td></tr></tbody></table></table></tables>

Referring to Fig. 6A to Fig. 6D, Fig. 6A illustrates the longitudinal spherical aberration of the third embodiment, and Fig. 6B and Fig. 6C respectively illustrate the third embodiment when the wavelength is 960 nm, 940 nm and 920 nm. The field curvature aberration in the sagittal direction and the field curvature aberration in the meridian direction on the imaging plane 100. The diagram in FIG. Distortion aberrations on . In the longitudinal spherical aberration diagram of the third embodiment shown in FIG. 6A , it can be seen from the deflection amplitude of each curve representing the wavelength that the imaging point deviation of off-axis rays at different heights is controlled within the range of ±0.025 mm. Therefore, the third embodiment does significantly improve spherical aberration at the same wavelength. In addition, the distances between the three representative wavelengths are quite close to each other, and the imaging positions representing different wavelengths of light are quite concentrated, so that the chromatic aberration is also significantly improved.

In the two field curvature aberration diagrams of Fig. 6B and Fig. 6C, the field curvature aberrations of the three representative wavelengths in the entire field of view fall within ±0.05 mm, which shows that the optical system of the third embodiment can effectively eliminate aberrations. The distortion aberration diagram in FIG. 6D shows that the distortion aberration of the third embodiment is maintained within the range of ±13%, indicating that the distortion aberration of the third embodiment meets the imaging quality requirements of the optical system. Compared with the existing imaging lens, the third embodiment can still provide good imaging quality under the condition that the total length of the lens is 55 mm, the aperture value is 1.45, the maximum image height is 8.5 mm, and some lenses are made of plastic lenses. In addition, in this embodiment, the F-theta distortion of the imaging lens 1000 is less than ±1%, indicating that it has good optical performance.

FIG. 7 is a schematic diagram of the imaging lens of the fourth embodiment of the present invention, and FIGS. 8A to 8D are diagrams of longitudinal spherical aberration and various aberrations of the imaging lens of the fourth embodiment. Please refer to FIG. 7 first. The imaging lens 1000 of the fourth embodiment of the present invention includes a first lens 1, a second lens 2, and a third lens along an optical axis I of the imaging lens 1000 from the object side A1 to the image side A2. 3. Aperture 0, fourth lens 4, fifth lens 5, sixth lens 6, seventh lens 7, filter 9 and cover glass 10, wherein the first lens 1, the third lens 3, and the fifth lens 5 And the seventh lens 7 is a glass lens, and the second lens 2 , the fourth lens 4 and the sixth lens 6 are plastic lenses. When the light emitted by an object to be photographed enters the imaging lens 1000, and passes through the first lens 1, the second lens 2, the third lens 3, the aperture 0, the fourth lens 4, the fifth lens 5, and the sixth lens 6. After the seventh lens 7 , the filter 9 and the cover glass 10 , an image will be formed on the imaging surface 100 . The filter 9 is, for example, an infrared pass filter. The filter 9 is disposed between the seventh lens 7 and the cover glass 10 .

In this embodiment, the first lens 1, second lens 2, third lens 3, fourth lens 4, fifth lens 5, sixth lens 6, seventh lens 7, filter 9 and The cover glass 10 all has the object side 15, 25, 35, 45, 55, 65, 75, 95, 105 facing the object side A1 and allowing the imaging light to pass through and the image side 16 facing the image side A2 and allowing the imaging light to pass through. 26, 36, 46, 56, 66, 76, 96, 106. In this embodiment, the aperture 0 is disposed between the third lens 3 and the fourth lens 4 .

The first lens 1 has a negative refractive power. Both the object side 15 and the image side 16 of the first lens 1 are spherical. The second lens 2 has a negative refractive power. Both the object side 25 and the image side 26 of the second lens 2 are aspherical. The third lens 3 has positive refractive power. Both the object side 35 and the image side 36 of the third lens 3 are spherical. The fourth lens 4 has a negative refractive power. Both the object side 45 and the image side 46 of the fourth lens 4 are aspherical. The fifth lens 5 has negative refractive power. Both the object side 55 and the image side 56 of the fifth lens 5 are spherical. The sixth lens 6 has positive refractive power. Both the object side 65 and the image side 66 of the sixth lens 6 are aspherical. The seventh lens 7 has positive refractive power. Both the object side 75 and the image side 76 of the seventh lens 7 are aspherical. According to an embodiment of the present invention, the seventh lens 7 is a glass molded lens.

Other detailed optical data of the fourth embodiment are shown in Table 7 below.

Table seven: <tables><table><table border="1" borderColor="#000000" width="85%"><tbody><tr><td>Fourth embodiment </td></tr><tr><td>Effective focal length = 14.2 mm, full field of view = 66°, overall lens length = 55.5 mm, aperture value = 1.29, maximum image height = 8.2 mm, overall lens length = 47.1 mm </td></tr><tr><td>element </td><td>noodle </td><td>Radius of curvature (mm) </td><td>spacing mm) </td><td>Refractive index </td><td>Abbe number </td></tr><tr><td>object </td><td> </td><td>Unlimited </td><td>Unlimited </td><td> </td><td> </td></tr><tr><td>first lens 1 </td><td>object side 15 </td><td>70.00 </td><td>1.00 </td><td>1.49 </td><td>70 </td></tr><tr><td> </td><td>like side 16 </td><td>11.14 </td><td>7.37 </td><td> </td><td> </td></tr><tr><td>second lens 2 </td><td>object side 25 </td><td>-13.76 </td><td>5.09 </td><td>1.64 </td><td>twenty four </td></tr><tr><td> </td><td>like profile 26 </td><td>-17.19 </td><td>0.08 </td><td> </td><td> </td></tr><tr><td>third lens 3 </td><td>object side 35 </td><td>18.50 </td><td>4.85 </td><td>1.83 </td><td>37 </td></tr><tr><td> </td><td>like side 36 </td><td>-83.73 </td><td>0.28 </td><td> </td><td> </td></tr><tr><td>Aperture 0 </td><td> </td><td>Unlimited </td><td>1.36 </td><td> </td><td> </td></tr><tr><td>Fourth lens 4 </td><td>object side 45 </td><td>14.42 </td><td>3.33 </td><td>1.64 </td><td>twenty four </td></tr><tr><td> </td><td>like side 46 </td><td>10.40 </td><td>8.28 </td><td> </td><td> </td></tr><tr><td>fifth lens 5 </td><td>object side 55 </td><td>-9.40 </td><td>2.73 </td><td>1.92 </td><td>twenty four </td></tr><tr><td> </td><td>like profile 56 </td><td>-13.96 </td><td>0.10 </td><td> </td><td> </td></tr><tr><td>sixth lens 6 </td><td>object side 65 </td><td>149.76 </td><td>5.97 </td><td>1.64 </td><td>twenty four </td></tr><tr><td> </td><td>like side 66 </td><td>-20.31 </td><td>0.09 </td><td> </td><td> </td></tr><tr><td>seventh lens 7 </td><td>object side 75 </td><td>16.33 </td><td>6.53 </td><td>1.73 </td><td>55 </td></tr><tr><td> </td><td>like side 76 </td><td>33.82 </td><td>5.06 </td><td> </td><td> </td></tr><tr><td>Filter 9 </td><td>object side 95 </td><td>Unlimited </td><td>0.40 </td><td>1.52 </td><td>64 </td></tr><tr><td> </td><td>like profile 96 </td><td>Unlimited </td><td>2.00 </td><td> </td><td> </td></tr><tr><td>cover glass 10 </td><td>object side 105 </td><td>Unlimited </td><td>0.50 </td><td>1.52 </td><td>64 </td></tr><tr><td> </td><td>like profile 106 </td><td>Unlimited </td><td>0.50 </td><td> </td><td> </td></tr><tr><td> </td><td>Imaging surface 100 </td><td>Unlimited </td><td>0.00 </td><td> </td><td> </td></tr></tbody></table></table></tables>

According to Table 7, the first lens 1 is a crescent lens with a convex surface facing the object side A1, the object side 15 is convex, and the image side 16 is concave. The second lens 2 is an aspherical lens with a convex surface facing the image side A2, the object side surface 25 is concave, and the image side surface 26 is convex. The third lens 3 is a biconvex lens, the object side 35 is convex, and the image side 36 is convex. The fourth lens 4 is an aspheric lens with a convex surface facing the object side A1, the object side 45 is convex, and the image side 46 is concave. The fifth lens 5 is a crescent lens with a convex surface facing the image side A2, the object side 55 is concave, and the image side 56 is convex. The sixth lens 6 is an aspherical lens with a convex object side 65 and a convex image side 66 . The seventh lens 7 is an aspheric lens with a convex surface facing the object side A1, the object side surface 75 is convex, and the image side 76 is concave.

The ratio of the thickness of the first lens 1 to the diameter is greater than 0.035, preferably greater than 0.04, the thickness refers to the thickness of the optical center of the first lens 1 on the optical axis I, and the diameter refers to the turning point between the first lens 1 optical center on both sides Taking this embodiment as an example, the thickness of the first lens is 1.00 mm, and the diameter is 23.43 mm. In addition, in this embodiment, the second lens 2, the fourth lens 4, the sixth lens 6, and the seventh lens 7 have eight object sides 25, 45, 65, 75 and image sides 26, 46, 66, 76 in total. The surfaces are all aspherical surfaces, and these aspheric surfaces are defined according to the above formula (1).

Two of the above-mentioned aspherical second lens 2, fourth lens 4, sixth lens 6, and seventh lens 7 can be selected, each of which can be replaced by two spherical lenses, so that the number of lenses in the lens is between 7 to 9 elements to avoid the problem of higher cost that may be caused by aspheric lenses. The various aspheric coefficients of the above-mentioned aspheric surface in formula (1) are shown in Table 8 below. Wherein, the column number 25 in Table 8 indicates that it is the aspheric coefficient of the object side surface 25 of the second lens 2, and the other columns can be deduced by analogy. In this embodiment, the 14th-order aspheric coefficient a of the above-mentioned aspheric surface 14are all zero.

Table Eight: <tables><table><table border="1" borderColor="#000000" width="85%"><tbody><tr><td>noodle </td><td>R </td><td>K </td><td>a 4 </td><td>a 6 </td></tr><tr><td>25 </td><td>-13.76 </td><td>-0.15 </td><td>3.97E-06 </td><td>-1.31E-07 </td></tr><tr><td>26 </td><td>-17.19 </td><td>-0.11 </td><td>-1.72E-06 </td><td>2.18E-09 </td></tr><tr><td>45 </td><td>14.42 </td><td>0.02 </td><td>-3.89E-05 </td><td>1.33E-07 </td></tr><tr><td>46 </td><td>10.40 </td><td>-0.31 </td><td>2.18E-05 </td><td>1.08E-08 </td></tr><tr><td>65 </td><td>149.76 </td><td>97.88 </td><td>4.69E-05 </td><td>3.30E-07 </td></tr><tr><td>66 </td><td>-20.31 </td><td>0.33 </td><td>5.70E-05 </td><td>3.16E-07 </td></tr><tr><td>75 </td><td>16.33 </td><td>-0.06 </td><td>0.00E+00 </td><td>0.00E+00 </td></tr><tr><td>76 </td><td>33.82 </td><td>2.04 </td><td>0.00E+00 </td><td>0.00E+00 </td></tr><tr><td>noodle </td><td>a 8 </td><td>a 10 </td><td>a 12 </td><td>a 14 </td></tr><tr><td>25 </td><td>1.34E-09 </td><td>0.00E+00 </td><td>0.00E+00 </td><td>0.00E+00 </td></tr><tr><td>26 </td><td>5.99E-10 </td><td>0.00E+00 </td><td>0.00E+00 </td><td>0.00E+00 </td></tr><tr><td>45 </td><td>-3.18E-09 </td><td>1.31E-11 </td><td>-3.16E-13 </td><td>0.00E+00 </td></tr><tr><td>46 </td><td>2.57E-08 </td><td>-5.06E-10 </td><td>4.95E-12 </td><td>0.00E+00 </td></tr><tr><td>65 </td><td>-3.13E-09 </td><td>1.87E-11 </td><td>-6.19E-14 </td><td>0.00E+00 </td></tr><tr><td>66 </td><td>-6.47E-10 </td><td>1.29E-11 </td><td>-7.62E-14 </td><td>0.00E+00 </td></tr><tr><td>75 </td><td>0.00E+00 </td><td>0.00E+00 </td><td>0.00E+00 </td><td>0.00E+00 </td></tr><tr><td>76 </td><td>0.00E+00 </td><td>0.00E+00 </td><td>0.00E+00 </td><td>0.00E+00 </td></tr></tbody></table></table></tables>

Referring again to FIG. 8A to FIG. 8D , FIG. 8A illustrates the longitudinal spherical aberration of the fourth embodiment, and FIG. 8B and FIG. 8C respectively illustrate the fourth embodiment when the wavelength is 960 nm, 940 nm and 920 nm. The field curvature aberration in the sagittal direction and the field curvature aberration in the meridian direction on the imaging plane 100. The diagram in FIG. Distortion aberrations on . In the longitudinal spherical aberration diagram of the fourth embodiment shown in FIG. 8A , it can be seen from the deflection amplitude of each curve representing the wavelength that the imaging point deviation of off-axis rays at different heights is controlled within the range of ±0.06 mm. Therefore, the fourth embodiment does significantly improve spherical aberration at the same wavelength. In addition, the distances between the three representative wavelengths are quite close to each other, and the imaging positions representing different wavelengths of light are quite concentrated, so that the chromatic aberration is also significantly improved.

In the two field curvature aberration diagrams of Fig. 8B and Fig. 8C, the field curvature aberrations of the three representative wavelengths in the entire field of view fall within ±0.08 mm, which shows that the optical system of the fourth embodiment can effectively eliminate aberrations. The distortion aberration diagram in FIG. 8D shows that the distortion aberration of the fourth embodiment is maintained within the range of ±12%, indicating that the distortion aberration of the fourth embodiment meets the imaging quality requirements of the optical system. Compared with the existing imaging lens, the fourth embodiment can still provide good imaging quality under the condition that the total length of the lens is 55.5 mm, the aperture value is 1.29, the maximum image height is 8.2 mm, and some lenses are made of plastic lenses. In addition, in this embodiment, the F-theta distortion of the imaging lens 1000 is less than ±0.22%, indicating that it has good optical performance.

FIG. 9 is a schematic diagram of an imaging lens according to a fifth embodiment of the present invention, and FIGS. 10A to 10D are graphs of longitudinal spherical aberration and various aberrations of the imaging lens according to the fifth embodiment. Please refer to FIG. 9 first. The imaging lens 1000 of the fifth embodiment of the present invention includes a first lens 1, a second lens 2, and a third lens along an optical axis I of the imaging lens 1000 from the object side A1 to the image side A2. 3. The fourth lens 4, the aperture 0, the fifth lens 5, the sixth lens 6, the seventh lens 7, the eighth lens 8 and the filter 9, wherein the first lens 1 to the eighth lens 8 are all glass lenses . When the light emitted by an object to be photographed enters the imaging lens 1000, and passes through the first lens 1, the second lens 2, the third lens 3, the fourth lens 4, the aperture 0, the fifth lens 5, and the sixth lens 6. After the seventh lens 7 , the eighth lens 8 and the filter 9 , an image will be formed on the imaging surface 100 . The filter 9 is, for example, an infrared pass filter.

In this embodiment, the first lens 1, the second lens 2, the third lens 3, the fourth lens 4, the fifth lens 5, the sixth lens 6, the seventh lens 7, the eighth lens 8 and the imaging lens 1000 The optical filters 9 all have respectively the object side faces 15, 25, 35, 45, 55, 65, 75, 85, 95 facing the object side A1 and allowing the imaging light to pass through and the image side 16 facing the image side A2 and allowing the imaging light to pass through , 26, 36, 46, 56, 66, 76, 86, 96. In this embodiment, the aperture 0 is disposed between the fourth lens 4 and the fifth lens 5 .

The imaging lens 1000 of this embodiment does not have a cemented lens. The first lens 1 has a negative refractive power. Both the object side 15 and the image side 16 of the first lens 1 are spherical. The second lens 2 has a negative refractive power. Both the object side 25 and the image side 26 of the second lens 2 are spherical. The third lens 3 has positive refractive power. Both the object side 35 and the image side 36 of the third lens 3 are spherical. The fourth lens 4 has positive refractive power. Both the object side 45 and the image side 46 of the fourth lens 4 are spherical. The fifth lens 5 has negative refractive power. Both the object side 55 and the image side 56 of the fifth lens 5 are spherical. The sixth lens 6 has negative refractive power. Both the object side 65 and the image side 66 of the sixth lens 6 are spherical. The seventh lens 7 has positive refractive power. Both the object side 75 and the image side 76 of the seventh lens 7 are aspherical. The eighth lens 8 has positive refractive power. Both the object side 85 and the image side 86 of the eighth lens 8 are spherical. According to an embodiment of the present invention, the seventh lens 7 is a glass molded lens.

Other detailed optical data of the fifth embodiment are shown in Table 9 below.

Table nine: <tables><table><table border="1" borderColor="#000000" width="85%"><tbody><tr><td>fifth embodiment </td></tr><tr><td>Effective focal length = 14.1 mm, full field of view = 66°, total lens length = 55 mm, aperture value = 1.5, Large image height = 8.1 mm, total lens length = 47.8 mm </td></tr><tr><td>element </td><td>noodle </td><td>Radius of curvature (mm) </td><td>spacing mm) </td><td>Refractive index </td><td>Abbe number </td></tr><tr><td>object </td><td> </td><td>Unlimited </td><td>Unlimited </td><td> </td><td> </td></tr><tr><td>first lens 1 </td><td>object side 15 </td><td>20.19 </td><td>1.20 </td><td>1.52 </td><td>64 </td></tr><tr><td> </td><td>like side 16 </td><td>10.45 </td><td>8.85 </td><td> </td><td> </td></tr><tr><td>second lens 2 </td><td>object side 25 </td><td>-13.64 </td><td>1.20 </td><td>1.55 </td><td>46 </td></tr><tr><td> </td><td>like profile 26 </td><td>34.44 </td><td>1.77 </td><td> </td><td> </td></tr><tr><td>third lens 3 </td><td>object side 35 </td><td>141.09 </td><td>4.90 </td><td>1.62 </td><td>63 </td></tr><tr><td> </td><td>like side 36 </td><td>-17.83 </td><td>0.10 </td><td> </td><td> </td></tr><tr><td>Fourth lens 4 </td><td>object side 45 </td><td>21.12 </td><td>4.96 </td><td>1.62 </td><td>63 </td></tr><tr><td> </td><td>like side 46 </td><td>-37.72 </td><td>2.20 </td><td> </td><td> </td></tr><tr><td>Aperture 0 </td><td> </td><td>Unlimited </td><td>0.10 </td><td> </td><td> </td></tr><tr><td>fifth lens 5 </td><td>object side 55 </td><td>11.45 </td><td>4.45 </td><td>1.83 </td><td>37 </td></tr><tr><td> </td><td>like profile 56 </td><td>8.53 </td><td>7.13 </td><td> </td><td> </td></tr><tr><td>sixth lens 6 </td><td>object side 65 </td><td>-8.96 </td><td>1.20 </td><td>1.81 </td><td>25 </td></tr><tr><td> </td><td>like side 66 </td><td>-17.34 </td><td>0.10 </td><td> </td><td> </td></tr><tr><td>seventh lens 7 </td><td>object side 75 </td><td>108.10 </td><td>4.50 </td><td>1.58 </td><td>59 </td></tr><tr><td> </td><td>like side 76 </td><td>-15.35 </td><td>0.10 </td><td> </td><td> </td></tr><tr><td>Eighth lens 8 </td><td>object side 85 </td><td>16.69 </td><td>5.00 </td><td>1.77 </td><td>50 </td></tr><tr><td> </td><td>like side 86 </td><td>48.48 </td><td>1.23 </td><td> </td><td> </td></tr><tr><td>Filter 9 </td><td>object side 95 </td><td>Unlimited </td><td>0.50 </td><td>1.52 </td><td>64 </td></tr><tr><td> </td><td>like profile 96 </td><td>Unlimited </td><td>5.50 </td><td> </td><td> </td></tr><tr><td> </td><td>Imaging surface 100 </td><td>Unlimited </td><td>0.00 </td><td> </td><td> </td></tr></tbody></table></table></tables>

According to Table 9, the first lens 1 is a crescent lens with a convex surface facing the object side A1, the object side 15 is convex, and the image side 16 is concave. The second lens 2 is a biconcave lens, the object side 25 is concave, and the image side 26 is concave. The third lens 3 is a biconvex lens, the object side 35 is convex, and the image side 36 is convex. The fourth lens 4 is a biconvex lens, the object side 45 is convex, and the image side 46 is concave. The fifth lens 5 is a crescent lens with a convex surface facing the object side A1, the object side 55 is convex, and the image side 56 is concave. The sixth lens 6 is a crescent lens with a convex surface facing the image side A2, the object side 65 is concave, and the image side 66 is convex. The seventh lens 7 is an aspheric lens, the object side 75 is convex, the image side 76 is convex in the optical axis region, and the circumference region is concave. The eighth lens 8 is a crescent lens with a convex surface facing the object side A1, the object side 85 is convex, and the image side 86 is concave.

The ratio of the thickness of the first lens 1 to the diameter is greater than 0.035, preferably greater than 0.04, the thickness refers to the thickness of the optical center of the first lens 1 on the optical axis I, and the diameter refers to the turning point between the first lens 1 optical center on both sides Taking this embodiment as an example, the thickness of the first lens is 1.20 mm, and the diameter is 24.19 mm. In addition, in this embodiment, both the object side 75 and the image side 76 of the seventh lens 7 are aspherical surfaces, and these aspheric surfaces are defined according to the above formula (1).

The above-mentioned aspheric seventh lens 7 can be replaced by two spherical lenses, so that the number of lenses of the lens is between 8 and 9, so as to avoid the problem of higher cost that may be caused by aspheric lenses. The various aspheric coefficients of the above-mentioned aspheric surface in formula (1) are shown in Table 10 below. Wherein, the column number 75 in Table 10 indicates that it is the aspheric coefficient of the object side 75 of the seventh lens 7 , and the column number 76 indicates that it is the aspheric coefficient of the image side 76 of the seventh lens 7 .

Table ten: <tables><table><table border="1" borderColor="#000000" width="85%"><tbody><tr><td>noodle </td><td>R </td><td>K </td><td>a 4 </td><td>a 6 </td></tr><tr><td>75 </td><td>0.01 </td><td>0.00 </td><td>1.25E-04 </td><td>1.20E-06 </td></tr><tr><td>76 </td><td>-0.07 </td><td>-0.72 </td><td>1.06E-04 </td><td>1.01E-06 </td></tr><tr><td>noodle </td><td>a 8 </td><td>a 10 </td><td>a 12 </td><td>a 14 </td></tr><tr><td>75 </td><td>-1.52E-08 </td><td>1.10E-10 </td><td>-2.52E-13 </td><td>0.00E+00 </td></tr><tr><td>76 </td><td>6.67E-09 </td><td>-4.18E-11 </td><td>2.84E-14 </td><td>0.00E+00 </td></tr></tbody></table></table></tables>

10A to 10D, FIG. 10A illustrates the longitudinal spherical aberration of the fifth embodiment, and FIG. 10B and FIG. 10C respectively illustrate the fifth embodiment when the wavelength is 960 nm, 940 nm and 920 nm. The field curvature aberration in the sagittal direction and the field curvature aberration in the meridian direction on the imaging plane 100. The diagram in FIG. Distortion aberrations on . In Fig. 10A of the longitudinal spherical aberration diagram of the fifth embodiment, it can be seen from the deflection amplitude of each curve representing the wavelength that the imaging point deviation of off-axis rays at different heights is controlled within the range of ±0.02 millimeters, Therefore, the fifth embodiment does significantly improve spherical aberration at the same wavelength. In addition, the distances between the three representative wavelengths are quite close to each other, and the imaging positions representing different wavelengths of light are quite concentrated, so that the chromatic aberration is also significantly improved.

In the two field curvature aberration diagrams of Fig. 10B and Fig. 10C, the field curvature aberrations of the three representative wavelengths in the entire field of view fall within ±0.05 mm, which shows that the optical system of the fifth embodiment can effectively eliminate aberrations. The distortion aberration diagram in FIG. 10D shows that the distortion aberration of the fifth embodiment is maintained within the range of ±12%, indicating that the distortion aberration of the fifth embodiment meets the imaging quality requirements of the optical system. Compared with the existing imaging lens, the fifth embodiment can still provide good imaging quality under the condition that the total length of the lens is 55 mm, the aperture value is 1.5 and the maximum image height is 8.1 mm. In addition, in this embodiment, the F-theta distortion of the imaging lens 1000 is less than ±0.8%, indicating that it has good optical performance.

In the above-mentioned first to fifth embodiments, 5, 6, 6, 7 and 8 lenses with diopters are provided respectively, but the present invention is not limited thereto. In other embodiments, 9 lenses with diopters can be provided.

FIG. 11 is a schematic diagram of the imaging lens of the sixth embodiment of the present invention, and FIGS. 12A to 12D are diagrams of longitudinal spherical aberration and various aberrations of the imaging lens of the sixth embodiment. Please refer to FIG. 11 first. The imaging lens 1000 of the sixth embodiment of the present invention includes a first lens 1, a second lens 2, an aperture 0, The third lens 3, the fourth lens 4, the fifth lens 5, the sixth lens 6, the seventh lens 7, the eighth lens 8 and the optical filter 9, wherein the first lens 1 to the eighth lens 8 are all glass lenses . When the light emitted by an object to be photographed enters the imaging lens 1000, and passes through the first lens 1, the second lens 2, the aperture 0, the third lens 3, the fourth lens 4, the fifth lens 5, and the sixth lens 6. After the seventh lens 7 , the eighth lens 8 and the filter 9 , an image will be formed on the imaging surface 100 . The filter 9 is, for example, an infrared pass filter.

The first lens 1 has positive refractive power. Both the object side 15 and the image side 16 of the first lens 1 are spherical. The second lens 2 has a negative refractive power. Both the object side 25 and the image side 26 of the second lens 2 are spherical. The third lens 3 has positive refractive power. Both the object side 35 and the image side 36 of the third lens 3 are spherical. The fourth lens 4 has positive refractive power. Both the object side 45 and the image side 46 of the fourth lens 4 are spherical. The fifth lens 5 has negative refractive power. Both the object side 55 and the image side 56 of the fifth lens 5 are spherical. The sixth lens 6 has positive refractive power. Both the object side 65 and the image side 66 of the sixth lens 6 are spherical. The seventh lens 7 has positive refractive power. Both the object side 75 and the image side 76 of the seventh lens 7 are spherical. The eighth lens 8 has positive refractive power. Both the object side 85 and the image side 86 of the eighth lens 8 are spherical.

Other detailed optical data of the sixth embodiment are shown in Table 11 below.

Table Eleven: <tables><table><table border="1" borderColor="#000000" width="85%"><tbody><tr><td>Sixth embodiment </td></tr><tr><td>Effective focal length = 14.1 mm, full field of view = 65°, total lens length = 55 mm, aperture value = 1.5, Large image height = 8.1 mm, total lens length = 49.9 mm </td></tr><tr><td>element </td><td>noodle </td><td>Radius of curvature (mm) </td><td>spacing mm) </td><td>Refractive index </td><td>Abbe number </td></tr><tr><td>object </td><td> </td><td>Unlimited </td><td>5.00E+04 </td><td> </td><td> </td></tr><tr><td>first lens 1 </td><td>object side 15 </td><td>16.19 </td><td>5.36 </td><td>1.99 </td><td>16 </td></tr><tr><td> </td><td>like side 16 </td><td>38.70 </td><td>1.02 </td><td> </td><td> </td></tr><tr><td>second lens 2 </td><td>object side 25 </td><td>30.32 </td><td>0.80 </td><td>1.70 </td><td>30 </td></tr><tr><td> </td><td>like profile 26 </td><td>7.48 </td><td>6.13 </td><td> </td><td> </td></tr><tr><td>Aperture 0 </td><td> </td><td>Unlimited </td><td>2.28 </td><td> </td><td> </td></tr><tr><td>third lens 3 </td><td>object side 35 </td><td>224.91 </td><td>2.41 </td><td>2.00 </td><td>29 </td></tr><tr><td> </td><td>like side 36 </td><td>-28.43 </td><td>0.51 </td><td> </td><td> </td></tr><tr><td>Fourth lens 4 </td><td>object side 45 </td><td>-19.57 </td><td>6.91 </td><td>1.69 </td><td>53 </td></tr><tr><td>fifth lens 5 </td><td>object side 55 </td><td>-18.68 </td><td>1.10 </td><td>1.52 </td><td>64 </td></tr><tr><td> </td><td>like profile 56 </td><td>58.09 </td><td>2.19 </td><td> </td><td> </td></tr><tr><td>sixth lens 6 </td><td>object side 65 </td><td>-60.54 </td><td>4.41 </td><td>2.00 </td><td>29 </td></tr><tr><td> </td><td>like side 66 </td><td>-19.93 </td><td>0.10 </td><td> </td><td> </td></tr><tr><td>seventh lens 7 </td><td>object side 75 </td><td>36.68 </td><td>5.26 </td><td>2.00 </td><td>29 </td></tr><tr><td> </td><td>like side 76 </td><td>-95.52 </td><td>2.91 </td><td> </td><td> </td></tr><tr><td>Eighth lens 8 </td><td>object side 85 </td><td>29.01 </td><td>8.50 </td><td>2.00 </td><td>29 </td></tr><tr><td> </td><td>like side 86 </td><td>25.85 </td><td>1.95 </td><td> </td><td> </td></tr><tr><td>Filter 9 </td><td>object side 95 </td><td>Unlimited </td><td>0.50 </td><td>1.52 </td><td>64 </td></tr><tr><td> </td><td>like profile 96 </td><td>Unlimited </td><td>2.66 </td><td> </td><td> </td></tr><tr><td> </td><td>Imaging surface 100 </td><td>Unlimited </td><td>0.00 </td><td> </td><td> </td></tr></tbody></table></table></tables>

Referring to FIG. 11 and Table 11, in this embodiment, the fourth lens 4 and the fifth lens 5 are cemented into a cemented lens, and the distance between the fourth lens 4 and the fifth lens 5 is less than or equal to 0.01 mm. Therefore, in Table 11, the radius of curvature of the object side 55 of the fifth lens 5 is also the radius of curvature of the image side of the fourth lens 4 .

According to Table 11, it can be known that the first lens 1 is a crescent lens with a convex surface facing the object side A1, the object side 15 is convex, and the image side 16 is concave. The second lens 2 is a crescent lens with a convex surface facing the object side A1, the object side 25 is convex, and the image side 26 is concave. The third lens 3 is a biconvex lens, the object side 35 is convex, and the image side 36 is convex. The fourth lens 4 is a crescent lens with a convex surface facing the image side A2, the object side 45 is concave, and the image side 46 is convex. The fifth lens 5 is a biconcave lens, the object side 55 is concave, and the image side 56 is concave. The sixth lens 6 is a crescent lens with a convex surface facing the image side A2, the object side 65 is concave, and the image side 66 is convex. The seventh lens 7 is a biconvex lens, the object side 75 is convex, and the image side 76 is convex. The eighth lens 8 is a crescent lens with a convex surface facing the object side A1, the object side 85 is convex, and the image side 86 is concave.

In this embodiment, the ratio of the thickness to the diameter of the first lens 1 is greater than 0.04, the thickness refers to the thickness of the optical center of the first lens 1 on the optical axis I, and the diameter refers to the distance between the turning points on both sides of the optical center of the first lens 1 distance. Taking this embodiment as an example, the first lens has a thickness of 5.36 mm and a diameter of 26.27 mm. The included angle between the chief ray of the imaging lens 1000 and the normal of the imaging surface 100 is less than 5°. The maximum image height is 8.3 mm. For light with a wavelength of 940 nm and a spatial frequency of 40 lp/mm (line log/mm), the modulation transfer function of the imaging lens 1000 is greater than 30%.

12A to 12D, FIG. 12A illustrates the longitudinal spherical aberration of the sixth embodiment, and the diagrams in FIG. 12B and FIG. 12C respectively illustrate the sixth embodiment when the wavelength is 960 nm, 940 nm and 920 nm. The field curvature aberration in the sagittal direction and the field curvature aberration in the meridian direction on the imaging plane 100. The diagram in FIG. Distortion aberrations on . In the longitudinal spherical aberration diagram of the sixth embodiment shown in FIG. 12A , it can be seen from the deflection amplitude of each curve representing the wavelength that the imaging point deviation of off-axis rays at different heights is controlled within the range of ±0.08 mm. Therefore, the sixth embodiment does significantly improve spherical aberration at the same wavelength. In addition, the distances between the three representative wavelengths are quite close to each other, and the imaging positions representing different wavelengths of light are quite concentrated, so that the chromatic aberration is also significantly improved.

In the two field curvature aberration diagrams of Fig. 12B and Fig. 12C, the field curvature aberrations of the three representative wavelengths in the entire field of view fall within ±0.08mm, which shows that the optical system of the sixth embodiment can effectively eliminate aberrations. The distortion aberration diagram in Figure 12D shows that the distortion aberration of the sixth embodiment is maintained within the range of ±10%, indicating that the distortion aberration of the sixth embodiment meets the imaging quality requirements of the optical system. Compared with the existing imaging lens, the sixth embodiment can still provide good imaging quality under the condition that the total length of the lens is 55 mm, the aperture value is 1.5, and the maximum image height is 8.1 mm.

1%. In this embodiment, the F-theta distortion of the imaging lens 1000 is less than ± 1.1%. The cone angle of light rays in each field of view is larger than 30°.

In the above-mentioned fifth and sixth embodiments, eight lenses with diopters are provided, but the present invention is not limited thereto. In other embodiments, 7 lenses with diopters can be provided, such as replacing two spherical lenses with an aspheric lens, or 9 lenses with diopters, such as replacing the aspheric lenses with two spherical lenses.

In summary, the imaging lens provided by the embodiment of the present invention satisfies the condition of Fno1.6 and has a large aperture. It also includes a glass lens for high temperature resistance. Imaging lens aberration is small. In addition, the included angle between the chief ray of the imaging lens and the normal of the imaging surface is less than 5°.

0: aperture , 2, 3, 4, 5, 6, 7, 8: lens : filter 0: cover glass 5, 25, 35, 45, 55, 65, 75, 85, 95, 105: object side 6, 26, 36, 46, 56, 66, 76, 86, 96, 106: side view 00: imaging surface 000: imaging lens 1: object side 2: image side : optical axis , Q: point

FIG. 1 is a schematic diagram of an imaging lens according to a first embodiment of the present invention. 2A to 2D are diagrams of longitudinal spherical aberration and various aberrations of the imaging lens in FIG. 1 . 3 is a schematic diagram of the imaging lens according to the second embodiment of the present invention. 4A to 4D are diagrams of longitudinal spherical aberration and various aberrations of the imaging lens in FIG. 3 . 5 is a schematic diagram of the imaging lens according to the third embodiment of the present invention. 6A to 6D are diagrams of longitudinal spherical aberration and various aberrations of the imaging lens in FIG. 5 . 7 is a schematic diagram of the imaging lens according to the fourth embodiment of the present invention. 8A to 8D are diagrams of longitudinal spherical aberration and various aberrations of the imaging lens in FIG. 7 . 9 is a schematic diagram of the imaging lens according to the fifth embodiment of the present invention. 10A to 10D are diagrams of longitudinal spherical aberration and various aberrations of the imaging lens in FIG. 9 . 11 is a schematic diagram of the imaging lens according to the sixth embodiment of the present invention. 12A to 12D are diagrams of longitudinal spherical aberration and various aberrations of the imaging lens of FIG. 11 .

Every citation, both ways

Citations
Document	Relation	Office	Cited during
US8416512B2	Cites	United States of America	Examiner
US8995062B2	Cites	United States of America	Examiner
TWI703367B	Cites	Taiwan Province of China	Examiner
TWI703367	Cites	Taiwan Province of China	–

2 members in 1 office

This recordMember, by publication date

Members2

Family members, oldest first
Document	Office	Kind
TWI802148BThis record	Taiwan Province of China	B	2023-05-11
TW202323917A	Taiwan Province of China	A	2023-06-16

Imaging lens

Abstract

Term

IMAGING LENS

Members2

Numbers

Titles2

Classification