TWI642988B - Optical lens assembly - Google Patents

Abstract

An optical lens group, the image side of the first lens having a concave portion located in the optical axis region and a concave portion located in the circumferential region. The second lens has a negative refractive power, and the object side has a concave surface located in the circumferential area. The object side of the third lens has a concave surface located in the circumferential area. The image side surface of the fourth lens has a convex portion located in the optical axis region and a convex portion located in the circumferential region. The fifth lens has a positive refractive power, and the image side has a concave surface located in the optical axis region. The image side surface of the sixth lens has a concave surface located in the optical axis region. ALT is the sum of the center thicknesses of the six lenses of the first lens to the sixth lens on the optical axis, the air gap on the optical axis between the fifth lens and the sixth lens is G56, and the center of the sixth lens on the optical axis The thickness is T6, which satisfies ALT/(G56+T6)≦2.6.

Description

Optical lens set

The present invention generally relates to an optical lens set. Specifically, the present invention particularly relates to an optical lens set mainly used for capturing images and video, and is used in portable electronic products, such as mobile phones, cameras, tablets, or personal digital assistants (Personal Digital). Assistant, PDA).

The specifications of consumer electronics are changing with each passing day. The pursuit of light and short steps has not slowed down. Therefore, the key components of electronic products such as optical lenses must be continuously improved in order to meet the needs of consumers. The most important feature of an optical lens is nothing more than image quality and volume. In the case of the six-piece lens structure, the conventional invention has a large distance from the side surface of the first lens to the imaging surface on the optical axis, which is disadvantageous for the thinning of the mobile phone and the digital camera.

In pursuit of lens thinning, it is necessary to take into account the quality and performance of the lens. Therefore, it is the main goal of the research to develop a lens with good imaging quality and thinness, and it is desirable to obtain a lens with good imaging quality and shortened lens length.

In view of this, the present invention thus proposes a six-piece optical lens set that reduces the system length of the optical lens, has good optical performance, and is technically feasible. The six-piece optical lens group of the present invention has a first lens, a second lens, a third lens, a fourth lens, a fifth lens, and a sixth lens arranged on the optical axis from the object side to the image side. Each of the first lens, the second lens, the third lens, the fourth lens, the fifth lens, and the sixth lens has an object side surface facing the object side and an image side surface facing the image side.

The image side surface of the first lens has a concave portion located in the vicinity of the optical axis, and also has a concave portion located in the vicinity of the circumference. The second lens has a negative refractive power, and the object side has a concave surface located in the vicinity of the circumference. The object side of the third lens has a concave surface located in the vicinity of the circumference. The image side surface of the fourth lens has a convex surface located in the vicinity of the optical axis, and also has a convex surface located in the vicinity of the circumference. The fifth lens has a positive refractive power, and the image side has a concave surface located in the vicinity of the optical axis. The image side surface of the sixth lens has a concave surface located in the vicinity of the optical axis. In the optical lens group, only the above six lenses having refractive power are used, and ALT is the sum of the center thicknesses of the six lenses of the first lens to the sixth lens on the optical axis, and the optical axis between the fifth lens and the sixth lens. The upper air gap is G56, the sixth lens has a center thickness on the optical axis of T6, and satisfies ALT/(G56+T6) ≦2.6.

In the optical lens group of the present invention, Tmax is the thickest single-piece thickness on the optical axis in the first lens to the sixth lens, and the air gap on the optical axis between the first lens and the second lens is G12, and satisfies Tmax/G12≦3.30.

In the optical lens group of the present invention, the air gap on the optical axis between the second lens and the third lens is G23, and satisfies Tmax/G23 ≦ 3.00.

In the optical lens group of the present invention, the center thickness of the first lens on the optical axis is T1, and satisfies (T1 + T6) / G12 ≦ 5.80.

In the optical lens group of the present invention, TTL is the length of the object side of the first lens to the imaging surface on the optical axis, the center thickness of the third lens on the optical axis is T3, and satisfies TTL/(T3+T6) ≦ 5.00 .

In the optical lens group of the present invention, the air gap of the third lens and the fourth lens on the optical axis is G34, and TTL / (G23 + G34) ≦ 8.70 is satisfied.

The optical lens set of the invention satisfies TTL/(G34+G56)≦5.10.

In the optical lens group of the present invention, the effective focal length of the optical lens system is EFL, the center thickness of the second lens on the optical axis is T2, and EFL/(T2+T6) ≦ 5.40 is satisfied.

The optical lens set of the present invention satisfies EFL/T2 ≦ 16.80.

In the optical lens group of the present invention, the BFL is the length of the image side of the sixth lens to the imaging plane on the optical axis, the center thickness of the fifth lens on the optical axis is T5, and satisfies BFL/T5 ≦ 3.00.

The optical lens set of the present invention satisfies BFL/T6 ≦ 2.00.

In the optical lens group of the present invention, Tmin is the thinnest single-piece thickness on the optical axis in the first lens to the sixth lens, and satisfies ALT/Tmin ≦ 9.70.

The optical lens set of the present invention satisfies ALT/G56≦4.30.

In the optical lens group of the present invention, Gmax is the largest air gap between the first lens and the sixth lens, and satisfies ALT/Gmax ≦ 4.50.

In the optical lens group of the present invention, TL is the distance from the object side of the first lens to the image side of the sixth lens on the optical axis, and satisfies TL/T6 ≦ 7.30.

In the optical lens group of the present invention, the air gap on the optical axis between the fourth lens and the fifth lens is G45, and satisfies TL / (G45 + G56) ≦ 5.80.

The optical lens set of the present invention satisfies TL/(T2+T6)≦5.10.

In the optical lens group of the present invention, the AAG is the sum of the five air gaps on the optical axis of the first lens to the sixth lens, and satisfies AAG/T2 ≦ 6.10.

The optical lens set of the present invention satisfies AAG/Tmin ≦ 6.10.

In the optical lens group of the present invention, the center thickness of the fourth lens on the optical axis is T4, and AAG/(T4 + T6) ≦ 1.90 is satisfied.

Before the present invention is described in detail, it is to be noted that in the drawings of the present invention, similar elements are denoted by the same reference numerals. Here, "a lens having a positive refractive power (or a negative refractive power)" as used in this specification means that the refractive index of the lens on the optical axis calculated by Gaussian optical theory is positive (or negative). ). The image side and the object side are defined as a range through which the imaging light passes, wherein the imaging light includes a chief ray Lc and a marginal ray Lm, as shown in FIG. 1, I is an optical axis and the lens is The optical axis I is symmetric with respect to each other in a radial direction. The region of the light passing through the optical axis is the region A near the optical axis, the region through which the edge light passes is the region C near the circumference, and the lens further includes an extension E ( That is, the radially outward region of the region C near the circumference, for the lens to be assembled in an optical lens group, the ideal imaging light does not pass through the extension portion E, but the structure and shape of the extension portion E are not In this regard, the following embodiments omits portions of the extensions for simplicity of the drawing. In more detail, the method of determining the area near the surface or the optical axis, the area near the circumference, or the range of the plurality of areas is as follows:

Please refer to FIG. 1, which is a cross-sectional view of a lens in the radial direction. In the cross-sectional view, when determining the range of the region, a center point is defined as an intersection with the optical axis on the surface of the lens, and a transition point is a point on the surface of the lens, and the line passing through the point It is perpendicular to the optical axis. If there are a plurality of transition points outward in the radial direction, the first transition point and the second transition point are sequentially, and the transition point farthest from the optical axis in the effective half-effect path is the Nth transition point. The range between the center point and the first transition point is a region near the optical axis, and the radially outward region of the Nth transition point is a region near the circumference, and different regions can be distinguished according to the respective transition points. Further, the effective radius is the vertical distance at which the edge ray Lm intersects the lens surface to the optical axis I.

As shown in FIG. 2, the shape concavities and convexities of the region are determined on the image side or the object side by the intersection of the light rays (or the light ray extending lines) passing through the region in parallel with the optical axis (the light focus determination method). For example, when the light passes through the area, the light will be focused toward the image side, and the focus of the optical axis will be on the image side, such as the R point in FIG. 2, and the area is a convex surface. Conversely, if the light passes through the certain area, the light will diverge, and the extension line and the focus of the optical axis are on the object side. For example, at point M in Fig. 2, the area is a concave surface, so the center point is between the first transition point. The convex portion, the radially outward portion of the first switching point is a concave surface; as can be seen from FIG. 2, the switching point is a boundary point of the convex surface of the convex surface, so that the inner side of the region adjacent to the radial direction can be defined. The area has a different face shape with the transition point as a boundary. In addition, if the shape of the region near the optical axis is judged according to the judgment of the person in the field, the R value (referring to the radius of curvature of the paraxial axis, generally refers to the R on the lens data in the optical software). Value) Positive and negative judgment bump. In the aspect of the object, when the R value is positive, it is determined as a convex surface, and when the R value is negative, it is determined as a concave surface; on the image side, when the R value is positive, it is determined as a concave surface, when R is When the value is negative, it is determined as a convex surface, and the unevenness determined by this method is the same as the light focus determination method. If there is no transition point on the surface of the lens, the area near the optical axis is defined as 0~50% of the effective radius, and the area near the circumference is defined as 50~100% of the effective radius.

The lens image side surface of the first example of Fig. 3 has only the first transition point on the effective radius, the first region is the vicinity of the optical axis, and the second region is the region near the circumference. The R value of the side of the lens image is positive, so that the area near the optical axis has a concave surface; the surface shape of the vicinity of the circumference is different from the inner area of the area immediately adjacent to the radial direction. That is, the area near the circumference and the area near the optical axis are different; the area near the circumference has a convex surface.

The lens object side surface of the example 2 of FIG. 4 has first and second switching points on the effective radius, and the first region is a region near the optical axis, and the third region is a region near the circumference. The R value of the side surface of the lens object is positive, so that the area near the optical axis is determined to be a convex surface; the area between the first switching point and the second switching point (second area) has a concave surface, and the area near the circumference (third area) Has a convex face.

The lens side surface of the third example of Fig. 5 has no transition point on the effective radius. At this time, the effective radius 0%~50% is the vicinity of the optical axis, and 50%~100% is the vicinity of the circumference. Since the R value in the vicinity of the optical axis is positive, the side surface of the object has a convex portion in the vicinity of the optical axis; and there is no transition point between the vicinity of the circumference and the vicinity of the optical axis, so that the vicinity of the circumference has a convex portion.

As shown in FIG. 6, the optical lens group 1 of the present invention includes an aperture 80, an optical aperture 40 from the object side 2 of the placed object (not shown) to the image side 3 of the image, along the optical axis 4. A lens 10, a second lens 20, a third lens 30, a fourth lens 40, a fifth lens 50, a sixth lens 60, a filter 70, and an image plane 71. In general, the first lens 10, the second lens 20, the third lens 30, the fourth lens 40, the fifth lens 50, and the sixth lens 60 may all be made of a transparent plastic material, but the present invention does not This is limited. Each lens has an appropriate refractive power. In the optical lens group 1 of the present invention, the lens having the refractive index has only six sheets of the first lens 10, the second lens 20, the third lens 30, the fourth lens 40, the fifth lens 50, and the sixth lens 60. Lens only. The optical axis 4 is the optical axis of the entire optical lens group 1, so that the optical axis of each lens and the optical axis of the optical lens group 1 are the same.

Further, the optical lens group 1 further includes an aperture stop 80 and is disposed at an appropriate position. In FIG. 6, the aperture 80 is disposed between the object side 2 and the first lens 10. When the light (not shown) emitted by the object to be photographed (not shown) on the object side 2 enters the optical lens group 1 of the present invention, the aperture 80, the first lens 10, the second lens 20, and the After the three lenses 30, the fourth lens 40, the fifth lens 50, the sixth lens 60, and the filter 70, they are focused on the imaging surface 71 of the image side 3 to form a clear image. In various embodiments of the present invention, the selectively disposed filter 70 may also be a filter having various suitable functions for filtering out light of a specific wavelength (for example, infrared rays), and is disposed on the side of the sixth lens 60 facing the image side. 62 is between the image plane 71.

Each of the lenses in the optical lens group 1 of the present invention has an object side surface facing the object side 2 and an image side surface facing the image side 3. Further, each of the lenses in the optical lens group 1 of the present invention also has a region near the optical axis close to the optical axis 4 and a region near the circumference away from the optical axis 4. For example, the first lens 10 has an object side surface 11 and an image side surface 12; the second lens 20 has an object side surface 21 and an image side surface 22; the third lens 30 has an object side surface 31 and an image side surface 32; and the fourth lens 40 has an object side surface 41 and The image side surface 42; the fifth lens 50 has an object side surface 51 and an image side surface 52; and the sixth lens 60 has an object side surface 61 and an image side surface 62. Each of the object side and the image side has a region near the optical axis close to the optical axis 4 and a region near the circumference away from the optical axis 4.

Each of the lenses in the optical lens set 1 of the present invention also has a center thickness T on the optical axis 4, respectively. For example, the first lens 10 has a first lens thickness T1, the second lens 20 has a second lens thickness T2, the third lens 30 has a third lens thickness T3, the fourth lens 40 has a fourth lens thickness T4, and the fifth lens 50 There is a fifth lens thickness T5, and the sixth lens 60 has a sixth lens thickness T6. Therefore, the sum of the center thicknesses of the lenses in the optical lens group 1 on the optical axis 4 is called ALT. That is, ALT = T1 + T2 + T3 + T4 + T5 + T6.

Further, in the optical lens group 1 of the present invention, an air gap located on the optical axis 4 is further provided between the respective lenses. For example, the air gap width between the first lens 10 and the second lens 20 is referred to as G12, the air gap width between the second lens 20 and the third lens 30 is referred to as G23, and the air between the third lens 30 and the fourth lens 40 is referred to as The gap width is referred to as G34, the air gap width between the fourth lens 40 and the fifth lens 50 is referred to as G45, and the air gap width between the fifth lens 50 and the sixth lens 60 is referred to as G56. Therefore, the sum of the total of five air gap widths between the first lens 10 and the sixth lens 60 between the lenses on the optical axis 4 is called AAG. That is, AAG = G12 + G23 + G34 + G45 + G56.

In addition, the length of the object side surface 11 to the imaging surface 71 of the first lens 10 on the optical axis 4 is TTL. The effective focal length of the optical lens group 14 is EFL, the length from the image side surface 62 of the sixth lens 60 to the imaging surface 71 on the optical axis 4 is BFL, and TL is the image side surface of the first lens 10 to the image side of the sixth lens 60. 62 is the length on the optical axis 4. Tmax is defined as the thickest single piece thickness on the optical axis 4 among the first lens 10, the second lens 20, the third lens 30, the fourth lens 40, the fifth lens 50, and the sixth lens 60. Tmin is defined as the thinnest single piece thickness on the optical axis 4 among the first lens 10, the second lens 20, the third lens 30, the fourth lens 40, the fifth lens 50, and the sixth lens 60.

In addition, it is further defined that f1 is the focal length of the first lens 10; f2 is the focal length of the second lens 20; f3 is the focal length of the third lens 30; f4 is the focal length of the fourth lens 40; f5 is the focal length of the fifth lens 50; F6 is the focal length of the sixth lens 60; n1 is the refractive index of the first lens 10; n2 is the refractive index of the second lens 20; n3 is the refractive index of the third lens 30; n4 is the refractive index of the fourth lens 40; n5 The refractive index of the fifth lens 50; n6 is the refractive index of the sixth lens 60; υ1 is the Abbe number of the first lens 10, that is, the dispersion coefficient; υ2 is the Abbe coefficient of the second lens 20; υ3 The Abbe's coefficient of the third lens 30; υ4 is the Abbe's coefficient of the fourth lens 10; υ5 is the Abbe's coefficient of the fifth lens 50; and υ6 is the Abbe's coefficient of the sixth lens 60.

First embodiment

Referring to Figure 6, a first embodiment of the optical lens assembly 1 of the present invention is illustrated. For the longitudinal spherical aberration on the imaging surface 71 of the first embodiment, please refer to FIG. 7A, the astigmatic field aberration in the sagittal direction, please refer to FIG. 7B and the tangential direction. Refer to Figure 7C for astigmatic aberrations and distortion aberration for reference. See Figure 7D. In all of the embodiments, the Y-axis of each of the spherical aberration diagrams represents the field of view, and the highest point is 1.0. In the embodiment, the astigmatism of the astigmatism and the distortion diagram represent the image height.

The optical lens group system 1 of the first embodiment is mainly composed of six lenses having a refractive power, a filter 70, a diaphragm 80, and an imaging surface 71. The aperture 80 is disposed between the object side 2 and the first lens 10. The filter 70 can prevent light of a specific wavelength (for example, infrared rays) from being projected onto an image plane to affect image quality.

The first lens 10 has a positive refractive power. The object side surface 11 facing the object side 2 has a convex portion 13 located in the vicinity of the optical axis and a convex portion 14 located in the vicinity of the circumference, and the image side surface 12 facing the image side 3 has the concave portion 16 located in the vicinity of the optical axis and located near the circumference The concave portion 17 of the region. Both the object side surface 11 and the image side surface 12 of the first lens are aspherical.

The second lens 20 has a negative refractive power. The object side surface 21 facing the object side 2 has a convex portion 23 located in the vicinity of the optical axis and a concave portion 24 located in the vicinity of the circumference, and the image side surface 22 facing the image side 3 has the concave portion 26 located in the vicinity of the optical axis and located near the circumference The concave portion 27 of the region. Both the object side surface 21 and the image side surface 22 of the second lens 20 are aspherical.

The third lens 30 has a positive refractive power, and the object side surface 31 facing the object side 2 has a convex portion 33 located in the vicinity of the optical axis and a concave portion 34 located in the vicinity of the circumference, and the image side 32 facing the image side 3 has the light in the side A convex portion 36 in the vicinity of the shaft and a convex portion 37 in the vicinity of the circumference. Further, the object side surface 31 and the image side surface 32 of the third lens 30 are both aspherical.

The fourth lens 40 has a negative refractive power, and the object side surface 41 facing the object side 2 has a concave portion 43 located in the vicinity of the optical axis and a concave portion 44 located in the vicinity of the circumference, and the image side 42 facing the image side 3 has the light in the side A convex portion 46 in the vicinity of the shaft and a convex portion 47 in the vicinity of the circumference. Further, the object side surface 41 and the image side surface 42 of the fourth lens 40 are both aspherical.

The fifth lens 50 has a positive refractive power, and the object side surface 51 facing the object side 2 has a convex portion 53 located in the vicinity of the optical axis and a concave portion 54 positioned near the circumference, and the image side surface 52 facing the image side 3 has the optical axis A concave portion 56 in the vicinity and a convex portion 57 located in the vicinity of the circumference. Further, the object side surface 51 and the image side surface 52 of the fifth lens 50 are both aspherical.

The sixth lens 60 has a negative refractive power, and the object side surface 61 facing the object side 2 has a convex portion 63 located in the vicinity of the optical axis and a concave portion 64 located in the vicinity of the circumference, and the image side surface 62 facing the image side 3 has the optical axis A concave portion 66 in the vicinity and a convex portion 67 located in the vicinity of the circumference. Further, the object side surface 61 and the image side surface 62 of the sixth lens 60 are both aspherical. The filter 70 is located between the image side surface 62 of the sixth lens 60 and the imaging surface 71.

In the optical lens group 1 of the present invention, from the first lens 10 to the sixth lens 60, the total side 11/21/31/41/51/61 and the image side 12/22/32/42/52/62 Twelve surfaces. If aspherical, these aspherical surfaces are defined by the following formula:

among them:

R represents the radius of curvature of the surface of the lens;

Z represents the depth of the aspherical surface (the point on the aspherical surface that is Y from the optical axis, and the tangent plane that is tangent to the vertex on the aspherical optical axis, the vertical distance between the two);

Y represents the vertical distance between the point on the aspherical surface and the optical axis;

K is a conic constant;

a _i is the i-th order aspheric coefficient.

The optical data of the optical lens system of the first embodiment is shown in Fig. 20, and the aspherical data is as shown in Fig.21. In the optical lens system of the following embodiments, the aperture value (f-number) of the integral optical lens system is Fno, the effective focal length is (EFL), and the Half Field of View (HFOV) is the largest in the overall optical lens system. Half of the Field of View, and the unit of curvature radius, thickness, and focal length are in millimeters (mm). The TTL is 4.982 mm, the Fno is 2.049, and the HFOV is 40.329 degrees.

Second embodiment

Referring to Figure 8, a second embodiment of the optical lens assembly 1 of the present invention is illustrated. It is to be noted that, from the second embodiment, in order to simplify and clearly express the drawings, only the faces of the lenses different from the first embodiment are specifically indicated on the drawings, and the remaining faces of the lenses of the first embodiment are For example, a concave or convex surface is not otherwise marked. For the longitudinal spherical aberration on the imaging surface 71 of the second embodiment, please refer to FIG. 9A, the astigmatic aberration in the sagittal direction, and FIG. 9B, the astigmatic aberration in the meridional direction, refer to FIG. 9C, and the distortion aberration, refer to FIG. 9D. . The design of the second embodiment is similar to that of the first embodiment, and only relevant parameters such as radius of curvature, lens refractive power, lens curvature radius, lens thickness, lens aspheric coefficient or back focus are different.

The detailed optical data of the second embodiment is shown in Fig. 22, and the aspherical data is as shown in Fig. 23. The TTL is 4.972 mm, the Fno is 2.059, and the HFOV is 39.016 degrees. In particular: 1. The lens length TTL of the second embodiment is shorter than that of the first embodiment. 2. The aperture Fno of the second embodiment is larger than that of the first embodiment. 3. The HFOV of the second embodiment is better than the first embodiment.

Third embodiment

Referring to Figure 10, a third embodiment of the optical lens assembly 1 of the present invention is illustrated. For the longitudinal spherical aberration on the imaging surface 71 of the third embodiment, please refer to FIG. 11A, the astigmatic aberration in the sagittal direction, and FIG. 11B, the astigmatic aberration in the meridional direction, refer to FIG. 11C, and the distortion aberration, refer to FIG. 11D. . The design of the third embodiment is similar to that of the first embodiment, and only relevant parameters such as radius of curvature, lens refractive power, lens curvature radius, lens thickness, lens aspheric coefficient or back focus are different.

The detailed optical data of the third embodiment is shown in Fig. 24, and the aspherical data is as shown in Fig. 25, the TTL is 4.814 mm, the Fno is 2.0588, and the HFOV is 42.3596 degrees. In particular: 1. The lens length TTL of the third embodiment is shorter than that of the first embodiment. 2. The aperture Fno of the third embodiment is larger than that of the first embodiment. 3. The HFOV of the third embodiment is better than the first embodiment.

Fourth embodiment

Referring to Figure 12, a fourth embodiment of the optical lens assembly 1 of the present invention is illustrated. For the longitudinal spherical aberration on the imaging surface 71 of the fourth embodiment, please refer to FIG. 13A, the astigmatic aberration in the sagittal direction, and FIG. 13B, the astigmatic aberration in the meridional direction, refer to FIG. 13C, and the distortion aberration, refer to FIG. 13D. . The design of the fourth embodiment is similar to that of the first embodiment, and only relevant parameters such as radius of curvature, lens power, lens curvature radius, lens thickness, lens aspheric coefficient or back focus are different.

The detailed optical data of the fourth embodiment is shown in Fig. 26. The aspherical data is as shown in Fig. 27, the TTL is 4.855 mm, the Fno is 2.0488, and the HFOV is 40.2938 degrees. In particular: 1. The lens length TTL of the fourth embodiment is shorter than that of the first embodiment.

Fifth embodiment

Referring to Figure 14, a fifth embodiment of the optical lens assembly 1 of the present invention is illustrated. For the longitudinal spherical aberration on the imaging surface 71 of the fifth embodiment, please refer to FIG. 15A, the astigmatic aberration in the sagittal direction, and FIG. 15B, the astigmatic aberration in the meridional direction, refer to FIG. 15C, and the distortion aberration, refer to FIG. 15D. . The design of the fifth embodiment is similar to that of the first embodiment, and only relevant parameters such as radius of curvature, lens refractive power, lens curvature radius, lens thickness, lens aspherical coefficient or back focus are different.

The detailed optical data of the fifth embodiment is shown in Fig. 28. The aspherical data is as shown in Fig. 29, the TTL is 4.99 mm, the Fno is 2.0487, and the HFOV is 40.335 degrees. In particular: 1. The HFOV of the fifth embodiment is better than the first embodiment.

Sixth embodiment

Referring to Figure 16, a sixth embodiment of the optical lens assembly 1 of the present invention is illustrated. For the longitudinal spherical aberration on the imaging surface 71 of the sixth embodiment, please refer to FIG. 17A, the astigmatic aberration in the sagittal direction, and FIG. 17B, the astigmatic aberration in the meridional direction, refer to FIG. 17C, and the distortion aberration, refer to FIG. 17D. . The design of the sixth embodiment is similar to that of the first embodiment except that only relevant parameters such as radius of curvature, lens power, lens radius of curvature, lens thickness, lens aspherical coefficient or back focus are different.

The detailed optical data of the sixth embodiment is shown in Fig. 30, and the aspherical data is as shown in Fig. 31, the TTL is 4.978 mm, the Fno is 2.0487, and the HFOV is 40.4391 degrees. In particular: 1. The lens length TTL of the sixth embodiment is shorter than that of the first embodiment. 2. The HFOV of the sixth embodiment is better than the first embodiment.

Seventh embodiment

Referring to Figure 18, a seventh embodiment of the optical lens assembly 1 of the present invention is illustrated. Please refer to FIG. 19A for the longitudinal spherical aberration on the imaging surface 71 of the seventh embodiment, FIG. 19B for the astigmatic aberration in the sagittal direction, FIG. 19C for the astigmatic aberration in the meridional direction, and FIG. 19D for the distortion aberration. . The design of the seventh embodiment is similar to that of the first embodiment, and only relevant parameters such as radius of curvature, lens refractive power, lens curvature radius, lens thickness, lens aspherical coefficient or back focus are different.

The detailed optical data of the seventh embodiment is shown in Fig. 32, and the aspherical data is as shown in Fig. 33, the TTL is 5.02 mm, the Fno is 2.0487, and the HFOV is 40.2916 degrees. The difference in thickness between the optical axis and the circumferential area of the lens of this embodiment is smaller than that of the first embodiment, and therefore it is easier to manufacture and the yield is higher.

In addition, the important parameters of the respective embodiments are organized in FIG. 34 and FIG. 35, respectively. Wherein TF represents the thickness of the filter 70 on the optical axis 4, GFP represents the gap width between the filter 70 and the imaging surface 71 on the optical axis 4, and BFL is the image side surface 62 of the sixth lens 60 to the imaging surface 71. The distance on the optical axis 4.

Applicant found that the lens configuration of this case has the following characteristics, and the corresponding effects that can be achieved:

The present invention carefully designs the vicinity of the optical axis of the lens and the vicinity of the circumference, wherein:

1. The first lens image side has a concave surface in the vicinity of the optical axis, and the vicinity of the circumference is a concave surface, which is favorable for light collection, the second lens has a negative refractive power and the second lens side has a circumferential vicinity. The concave surface is easy to correct the first lens to produce the main aberration.

2. The convex surface of the side surface of the third lens object in the vicinity of the circumference and the side surface of the fourth lens image in the vicinity of the optical axis and the vicinity of the circumference are favorable for correcting the main aberration of the front lens and improving the image quality.

3. The fifth lens has a positive refractive power and the fifth lens image side has a concave surface correctable aberration in the vicinity of the optical axis, and the sixth lens image side has a concave surface in the vicinity of the optical axis. Design, the above design works together to shorten the lens length while ensuring image quality.

In order to shorten the length of the lens system, the present invention appropriately shortens the lens thickness and the air gap between the lenses, but considering the difficulty of the lens assembly process and the necessity of taking into consideration the image quality, the lens thickness and the air gap between the lenses need to be mutually The configuration is such that the optical imaging system can achieve a better configuration under the numerical limits that satisfy the following conditional formula. In addition, through the numerical control of the following parameters, the designer can assist the designer to design a technically feasible optical lens set with good optical performance. The ratio of different parameters has a better range.

When the optical imaging lens of the present invention satisfies any of the following conditional expressions, it means that when the denominator is constant, the length of the molecule can be relatively shortened, and the effect of reducing the volume of the lens can be achieved: if any of the following conditional expressions can be further obtained, Better image quality:

ALT / (G56 + T6) ≦ 2.60, a preferred range is 1.90 ≦ ALT / (G56 + T6) ≦ 2.60;

Tmax/G12≦3.30, preferably 2.80≦Tmax/G12≦3.30;

Tmax/G23 ≦ 3.00, preferably in the range of 2.50 ≦ Tmax / G23 ≦ 3.00;

(T1+T6)/G12≦5.80, the preferred range is 5.50≦(T1+T6)/G12≦5.80;

BFL/T5 ≦ 3.00, preferably in the range of 2.00 ≦ BFL / T5 ≦ 3.00;

BFL/T6 ≦ 2.00, preferably in the range of 1.30 ≦ BFL / T6 ≦ 2.00;

ALT/Tmin ≦ 9.70, preferably in the range 9.40 ≦ ALT / Tmin ≦ 9.70;

ALT/G56≦4.30, the preferred range is 3.60≦ALT/G56≦4.30;

ALT/Gmax ≦ 4.50, preferably in the range of 3.60 ≦ ALT / Gmax ≦ 4.50;

TL/T6≦7.30, the preferred range is 6.30≦TL/T6≦7.30;

TL / (G45 + G56) ≦ 5.80, a preferred range is 5.10 ≦ TL / (G45 + G56) ≦ 5.80;

TL / (T2 + T6) ≦ 5.10, a preferred range is 4.40 ≦ TL / (T2 + T6) ≦ 5.10;

AAG/T2≦6.10, the preferred range is 5.30≦AAG/T2≦6.10;

AAG/Tmin≦6.10, preferably in the range of 5.50≦AAG/Tmin≦6.10;

AAG/(T4+T6) ≦ 1.90, preferably in the range of 1.60 ≦ AAG / (T4 + T6) ≦ 1.90.

Shortening the EFL contributes to the expansion of the viewing angle, so the EFL is designed to be smaller. If the following conditional expression is satisfied, the angle of the field of view can also be increased during the thinning of the optical system.

EFL / (T2 + T6) ≦ 5.40, a preferred range is 4.30 ≦ EFL / (T2 + T6) ≦ 5.40;

EFL/T2 ≦ 16.80, the preferred range is 14.40 ≦ EFL / T2 ≦ 16.80.

Maintaining an appropriate value between the optical component parameters and the lens length ratio, avoiding too small a parameter is not conducive to manufacturing, or avoiding excessive parameters and making the lens length too long.

TTL / (T3 + T6) ≦ 5.00, the preferred range is 4.40 ≦ TTL / (T3 + T6) ≦ 5.00;

TTL / (G23 + G34) ≦ 8.70, the preferred range is 8.30 ≦ TTL / (G23 + G34) ≦ 8.70;

TTL / (G34 + G56) ≦ 5.10, the preferred range is 4.60 ≦ TTL / (G34 + G56) ≦ 5.10.

In view of the unpredictability of optical system design, under the framework of the present invention, the above conditional condition can better shorten the lens length, increase the available aperture, increase the angle of view, improve the imaging quality, or assemble well. The rate is improved to improve the shortcomings of the prior art.

In addition, any combination of the parameters of the embodiment can be selected to increase the lens limit to facilitate the lens design of the same architecture of the present invention. In view of the unpredictability of the optical system design, under the framework of the present invention, the above conditional condition can better improve the depth of the telescope head of the present invention, increase the available aperture, improve the imaging quality, or improve the assembly yield. The disadvantages of the prior art.

The exemplary defined relationship listed above may also be arbitrarily combined and applied in an unequal amount in the embodiment of the present invention, and is not limited thereto. In the implementation of the present invention, in addition to the foregoing relationship, a fine structure such as a concave-convex surface arrangement of a plurality of other lenses may be additionally designed for a single lens or a plurality of lenses to enhance system performance and/or For the control of the resolution, for example, a convex portion located in the vicinity of the optical axis may be additionally additionally formed on the object side of the first lens. It should be noted that such details need to be selectively combined and applied to other embodiments of the invention without conflict.

The longitudinal spherical aberration, astigmatic aberration, and distortion of the embodiments of the present invention all conform to the usage specifications. In addition, the three off-axis rays of different wavelengths of red, green and blue are concentrated near the imaging point. The deviation of the amplitude of each curve shows that the deviation of the imaging points of the off-axis rays of different heights is controlled. Good spherical aberration, aberration, and distortion suppression. Referring further to the imaging quality data, the distances of the three representative wavelengths of red, green and blue are also relatively close to each other, indicating that the present invention has excellent concentration and suppression of different wavelengths of light in various states. In summary, the present invention can produce excellent image quality by designing and matching the lenses. The above are only the preferred embodiments of the present invention, and all changes and modifications made to the scope of the present invention should be within the scope of the present invention.

1‧‧‧Optical lens group

2‧‧‧ object side

3‧‧‧ image side

4‧‧‧ optical axis

10‧‧‧ first lens

11‧‧‧ ‧ side

12‧‧‧like side

13‧‧‧ convex face

14‧‧‧ convex face

16‧‧‧ concave face

17‧‧‧ concave face

20‧‧‧second lens

21‧‧‧ ‧ side

22‧‧‧like side

23‧‧‧ convex face

24‧‧‧ concave face

26‧‧‧ concave face

27‧‧‧ concave face

30‧‧‧ third lens

31‧‧‧ ‧ side

32‧‧‧like side

33‧‧‧ convex face

34‧‧‧ concave face

36‧‧‧ convex face

37‧‧‧ convex face

40‧‧‧Fourth lens

41‧‧‧ ‧ side

42‧‧‧like side

43‧‧‧ concave face

44‧‧‧ concave face

46‧‧‧ convex face

47‧‧‧ convex face

50‧‧‧ fifth lens

51‧‧‧ ‧ side

52‧‧‧like side

53‧‧‧ convex face

54‧‧‧ concave face

56‧‧‧ concave face

57‧‧‧ convex face

60‧‧‧ sixth lens

61‧‧‧ ‧ side

62‧‧‧like side

63‧‧‧ convex face

64‧‧‧ concave face

66‧‧‧ concave face

67‧‧‧ convex face

70‧‧‧Filter

71‧‧‧ imaging surface

80‧‧‧ aperture

T1~T6‧‧‧ lens center thickness

I‧‧‧ optical axis

A~C‧‧‧Area

E‧‧‧Extension

Lc‧‧‧ chief ray

Lm‧‧‧ edge light

1 to 5 are schematic views showing a method of determining a curvature shape of an optical lens group of the present invention. 6 is a schematic view showing a first embodiment of a seven-piece optical lens unit of the present invention. Fig. 7A illustrates the longitudinal spherical aberration on the image plane of the first embodiment. Fig. 7B illustrates the astigmatic aberration in the sagittal direction of the first embodiment. Fig. 7C illustrates the astigmatic aberration in the meridional direction of the first embodiment. Fig. 7D illustrates the distortion aberration of the first embodiment. Figure 8 is a schematic view showing a second embodiment of the seven-piece optical lens unit of the present invention. Figure 9A illustrates the longitudinal spherical aberration on the image plane of the second embodiment. FIG. 9B illustrates the astigmatic aberration in the sagittal direction of the second embodiment. Fig. 9C illustrates the astigmatic aberration in the meridional direction of the second embodiment. Fig. 9D illustrates the distortion aberration of the second embodiment. Figure 10 is a schematic view showing a third embodiment of the seven-piece optical lens unit of the present invention. Figure 11A illustrates the longitudinal spherical aberration on the image plane of the third embodiment. Fig. 11B illustrates the astigmatic aberration in the sagittal direction of the third embodiment. Fig. 11C illustrates the astigmatic aberration in the meridional direction of the third embodiment. Fig. 11D illustrates the distortion aberration of the third embodiment. Figure 12 is a schematic view showing a fourth embodiment of the seven-piece optical lens unit of the present invention. Figure 13A illustrates the longitudinal spherical aberration on the image plane of the fourth embodiment. Fig. 13B illustrates the astigmatic aberration in the sagittal direction of the fourth embodiment. Fig. 13C illustrates the astigmatic aberration in the meridional direction of the fourth embodiment. Fig. 13D illustrates the distortion aberration of the fourth embodiment. Figure 14 is a schematic view showing a fifth embodiment of the seven-piece optical lens unit of the present invention. Figure 15A illustrates the longitudinal spherical aberration on the image plane of the fifth embodiment. Fig. 15B illustrates the astigmatic aberration in the sagittal direction of the fifth embodiment. Fig. 15C illustrates the astigmatic aberration in the meridional direction of the fifth embodiment. Fig. 15D illustrates the distortion aberration of the fifth embodiment. Figure 16 is a schematic view showing a sixth embodiment of the seven-piece optical lens unit of the present invention. Figure 17A illustrates the longitudinal spherical aberration on the image plane of the sixth embodiment. Fig. 17B illustrates the astigmatic aberration in the sagittal direction of the sixth embodiment. Fig. 17C shows the astigmatic aberration in the meridional direction of the sixth embodiment. Fig. 17D illustrates the distortion aberration of the sixth embodiment. Figure 18 is a schematic view showing a seventh embodiment of the seven-piece optical lens unit of the present invention. Figure 19A illustrates the longitudinal spherical aberration on the image plane of the seventh embodiment. Fig. 19B illustrates the astigmatic aberration in the sagittal direction of the seventh embodiment. Fig. 19C shows the astigmatic aberration in the tangential direction of the seventh embodiment. Fig. 19D illustrates the distortion aberration of the seventh embodiment. Fig. 20 shows the detailed optical data of the first embodiment. Fig. 21 shows detailed aspherical data of the first embodiment. Fig. 22 shows detailed optical data of the second embodiment. Fig. 23 shows detailed aspherical data of the second embodiment. Fig. 24 shows detailed optical data of the third embodiment. Fig. 25 shows detailed aspherical data of the third embodiment. Fig. 26 shows detailed optical data of the fourth embodiment. Fig. 27 shows detailed aspherical data of the fourth embodiment. Fig. 28 shows detailed optical data of the fifth embodiment. Fig. 29 shows detailed aspherical data of the fifth embodiment. Fig. 30 shows detailed optical data of the sixth embodiment. Fig. 31 shows detailed aspherical data of the sixth embodiment. Fig. 32 shows detailed optical data of the seventh embodiment. Fig. 33 shows detailed aspherical data of the seventh embodiment. Figure 34 shows the important parameters of the various embodiments. Figure 35 shows the important parameters of the various embodiments.

Claims (19)

An optical lens group comprising a first lens, a second lens, a third lens, a fourth lens, a fifth lens and a sixth lens sequentially along an optical axis from an object side to an image side, Each lens has an object side surface facing the object side and an image side surface facing the image side. The optical lens group includes: the image side surface of the first lens has a concave surface located in the vicinity of the optical axis, and has a circumference a concave portion in the vicinity; the second lens has a negative refractive power, the object side has a concave portion in the vicinity of the circumference; the object side of the third lens has a concave portion in the vicinity of the circumference; The image side surface of the lens has a convex portion located in the vicinity of the optical axis, and a convex portion having a region in the vicinity of the circumference; the fifth lens has a positive refractive power, and the image side has a concave portion located in the vicinity of the optical axis And the image side of the sixth lens has a concave surface located in the vicinity of the optical axis; wherein the optical lens group has only the above six lenses having refractive power, and ALT is the first lens The sum of the center thicknesses of the six lenses on the optical axis of the sixth lens, Gmax being the largest air gap between the first lens and the sixth lens, and the optical axis between the fifth lens and the sixth lens The upper air gap is G56, the center thickness of the sixth lens on the optical axis is T6, and satisfies ALT/(G56+T6) ≦ 2.6, and ALT/Gmax ≦ 4.50. The optical lens set of claim 1, wherein Tmax is the thickest single piece thickness of the first lens to the sixth lens on the optical axis, and the first lens and the second lens are on the optical axis An air gap is G12 and satisfies Tmax/G12 ≦ 3.30. The optical lens set of claim 1, wherein Tmax is the thickest single piece thickness on the optical axis of the first lens to the sixth lens, and the optical axis is between the second lens and the third lens An air gap is G23 and satisfies Tmax/G23 ≦ 3.00. The optical lens set of claim 1, wherein a center thickness of the first lens on the optical axis is T1, and an air gap between the first lens and the second lens on the optical axis is G12, and is satisfied ( T1+T6)/G12≦5.80. The optical lens set of claim 1, wherein the TTL is the length of the object side of the first lens to an imaging surface on the optical axis, the center thickness of the third lens on the optical axis is T3, and the TTL is satisfied. /(T3+T6)≦5.00. The optical lens set of claim 1, wherein the TTL is a length of the object side of the first lens to an imaging surface on the optical axis, and a relationship between the second lens and the third lens on the optical axis The air gap is G23, an air gap of the third lens and the fourth lens on the optical axis is G34, and TTL / (G23 + G34) ≦ 8.70 is satisfied. The optical lens set of claim 1, wherein TTL is a length of the object side of the first lens to an imaging surface on the optical axis, and an air gap of the third lens and the fourth lens on the optical axis It is G34 and meets TTL/(G34+G56)≦5.10. The optical lens set of claim 1, wherein the optical lens set has an effective focal length of EFL, a center thickness of the second lens on the optical axis is T2, and satisfies EFL/(T2+T6) ≦ 5.40. The optical lens set of claim 1, wherein the optical lens group has an effective focal length of EFL, a center thickness of the second lens on the optical axis is T2, and satisfies EFL/T2 ≦ 16.80. The optical lens set of claim 1, wherein the BFL is the length of the image side of the sixth lens to an imaging surface on the optical axis, the center thickness of the fifth lens on the optical axis is T5, and the BFL is satisfied. /T5≦3.00. The optical lens set of claim 1, wherein the BFL is the length of the image side of the sixth lens to an imaging surface on the optical axis, and satisfies BFL/T6 ≦ 2.00. The optical lens set of claim 1, wherein Tmin is the thinnest single piece thickness on the optical axis of the first lens to the sixth lens, and satisfies ALT/Tmin ≦ 9.70. The optical lens set of claim 1 satisfies ALT/G56≦4.30. The optical lens set of claim 1, wherein TL is a distance from the object side of the first lens to the image side of the sixth lens on the optical axis, and satisfies TL/T6 ≦ 7.30. The optical lens set of claim 1, wherein TL is a distance from the side of the object of the first lens to the image side of the sixth lens on the optical axis, and between the fourth lens and the fifth lens An air gap on the optical axis is G45 and satisfies TL/(G45+G56) ≦ 5.80. The optical lens set of claim 1, wherein TL is a distance from the object side of the first lens to the image side of the sixth lens on the optical axis, and a center thickness of the second lens on the optical axis is T2, and satisfies TL/(T2+T6)≦5.10. The optical lens set of claim 1, wherein the AAG is a sum of five air gaps on the optical axis of the first lens to the sixth lens, and a center thickness of the second lens on the optical axis is T2, and satisfies AAG/T2≦6.10. The optical lens set of claim 1, wherein the AAG is a sum of five air gaps on the optical axis of the first lens to the sixth lens, and Tmin is the first lens to the sixth lens on the optical axis The thinnest single piece thickness and meets AAG/Tmin≦6.10. The optical lens set of claim 1, wherein AAG is a sum of five air gaps of the first lens to the sixth lens on the optical axis, a center thickness of the fourth lens on the optical axis is T4, and satisfies AAG/(T4+T6) ≦ 1.90.