CN211402904U

CN211402904U - Camera optical lens

Info

Publication number: CN211402904U
Application number: CN202020131678.4U
Authority: CN
Inventors: 曹来书; 李雪慧
Original assignee: Xiamen Leading Optics Co Ltd
Current assignee: Xiamen Leading Optics Co Ltd
Priority date: 2020-01-20
Filing date: 2020-01-20
Publication date: 2020-09-01
Anticipated expiration: 2030-01-20

Abstract

The utility model discloses a camera optical lens, which comprises a first lens, a second lens, a third lens, a diaphragm, a fourth lens, a fifth lens and a sixth lens from an object side to an image side in sequence; the first lens is a convex-concave glass spherical lens, and the focal length is negative; the second lens is a plastic aspheric surface, and the focal length is negative; the third lens is a biconvex glass spherical surface, and the focal length is positive; the fourth lens and the fifth lens are cemented lenses, the fourth lens is a convex-concave negative lens, the fifth lens is a double-convex positive lens, and the focal length is positive after the cementing; the sixth lens is a plastic aspheric surface, and the focal length is positive. The utility model provides a technical scheme optical lens distortion of making a video recording reaches and is greater than 18%, in the same unit angle of vision, the edge distribution pixel is more than the center, and the edge object is shown to the salient to use 4G2P structure, at the high low temperature center out of focus condition, satisfy the edge and can not produce the field curvature problem.

Description

Camera optical lens

Technical Field

The utility model belongs to the technical field of the camera lens, specifically relate to an optical lens makes a video recording.

Background

A fisheye lens is a lens having a focal length of 16mm or less and a viewing angle close to or equal to 180 °. It is an extreme wide-angle lens, and the "fish-eye lens" is its common name. In order to maximize the angle of view of the lens, the front lens of the lens is short in diameter and is parabolic and convex toward the front of the lens, much like the fish eye, so called "fish-eye lens".

The fisheye lens belongs to a special lens in an ultra-wide angle lens, and the visual angle of the fisheye lens is required to reach or exceed the range which can be seen by human eyes. Therefore, the fisheye lens is very different from the real world scene in human eyes, because the scene seen in real life is in a regular fixed form, and the picture effect generated by the fisheye lens is beyond the scope.

In a general imaging optical lens, the f-theta distortion is negative, the edge distortion is negative, and the number of pixels distributed on the edge is small at the same unit field angle. The traditional positive distortion image pickup optical lens has obvious stray light ghost image in a strong light environment; and the positive distortion image pickup optical lens uses more plastic aspheric surfaces, the plastic aspheric surfaces are more, and the problem of edge field curvature occurs at high and low temperature.

SUMMERY OF THE UTILITY MODEL

An object of the utility model is to provide a camera optical lens.

In order to achieve the above object, the utility model adopts the following technical scheme: a photographic optical lens comprises a first lens, a second lens, a third lens, a diaphragm, a fourth lens, a fifth lens and a sixth lens from an object side to an image side in sequence;

the first lens is a convex-concave glass spherical lens, and the focal length is negative;

the second lens is a plastic aspheric surface, and the focal length is negative;

the third lens is a biconvex glass spherical surface, and the focal length is positive;

the fourth lens and the fifth lens are cemented lenses, the fourth lens is a convex-concave negative lens, the fifth lens is a double-convex positive lens, and the focal length is positive after the cementing;

the sixth lens is a plastic aspheric surface, and the focal length is positive.

Preferably, the imaging optical lens further satisfies: 2< | f2/f | <3, and 3< | f3/f | <4, where f is the system focal length, f2 is the focal length of the second lens, and f3 is the focal length of the third lens.

Preferably, the imaging optical lens further satisfies: 4.5< | f45/f | <6, and 5< | f6/f | <6, where f is the focal length of the system, f45 is the focal length of the fourth lens and the fifth lens after being focused, and f6 is the focal length of the sixth lens.

Preferably, the imaging optical lens further satisfies: 0.37< | f2/f6| < 0.55.

Preferably, an aluminum spacer ring is used between the optical system lenses to match a metal frame, and a metal aluminum support seat is used for each lens.

Preferably, the high temperature of the lens causes the back focus to change, denoted as Δ BFL1, the metal aluminum support seat causes the back focus to change, denoted as Δ BFL2, Δ BFL1- Δ BFL2 are close to 0.

The utility model has the advantages of:

the utility model adopts six lenses, the positive f-theta distortion reaches more than 18 percent by correspondingly designing each lens, the edge distribution pixels are more than the center at the same unit field angle, and edge objects are highlighted; the positive f-theta distortion image pickup optical lens is weak in stray light ghost image, and the contrast of the whole picture is improved; the positive f-theta distortion image pickup optical lens adopts a 4G2P (namely, 4 glass lenses and 2 plastic lenses) structure, so that the field curvature problem can not be generated at the edge under the condition of no defocusing at the high and low temperature center.

Drawings

In order to more clearly illustrate the technical solutions in the embodiments of the present invention, the drawings needed to be used in the description of the embodiments will be briefly described below, and it is obvious that the drawings in the following description are only some embodiments of the present invention, and for those skilled in the art, other drawings can be obtained according to these drawings without creative efforts.

Fig. 1 is a schematic structural diagram of an embodiment of the present invention;

fig. 2 is a defocus graph according to the first embodiment of the present invention;

fig. 3 is a distortion curve diagram of the first embodiment of the present invention;

fig. 4 is a vertical axis aberration diagram according to a first embodiment of the present invention;

fig. 5 is a lateral chromatic aberration diagram according to a first embodiment of the present invention;

fig. 6 is a defocus graph of the second embodiment of the present invention;

fig. 7 is a distortion curve diagram of a second embodiment of the present invention;

fig. 8 is a vertical axis aberration diagram according to the second embodiment of the present invention;

fig. 9 is a lateral chromatic aberration diagram according to a second embodiment of the present invention;

fig. 10 is a defocus graph of a third embodiment of the present invention;

fig. 11 is a distortion curve diagram of a third embodiment of the present invention;

fig. 12 is a vertical axis aberration diagram according to a third embodiment of the present invention;

fig. 13 is a lateral chromatic aberration diagram according to a third embodiment of the present invention;

fig. 14 is a defocus graph of the fourth embodiment of the present invention;

fig. 15 is a distortion curve diagram of a fourth embodiment of the present invention;

fig. 16 is a vertical axis aberration diagram according to a fourth embodiment of the present invention;

fig. 17 is a lateral chromatic aberration diagram according to a fourth embodiment of the present invention;

fig. 18 is a defocus graph of the fifth embodiment of the present invention;

fig. 19 is a distortion curve diagram of embodiment five of the present invention;

fig. 20 is a vertical axis aberration diagram according to fifth embodiment of the present invention;

fig. 21 is a lateral chromatic aberration diagram according to a fifth embodiment of the present invention.

Detailed Description

To further illustrate the embodiments, the present invention provides the accompanying drawings. The accompanying drawings, which are incorporated in and constitute a part of this disclosure, illustrate embodiments of the invention and, together with the description, serve to explain the principles of the embodiments. With these references, one of ordinary skill in the art will appreciate other possible embodiments and advantages of the present invention. Elements in the figures are not drawn to scale and like reference numerals are generally used to indicate like elements.

The present invention will now be further described with reference to the accompanying drawings and detailed description.

The phrase "a lens element has a positive refractive index (or a negative refractive index)" means that the paraxial refractive index of the lens element calculated by Gaussian optics theory is positive (or negative). The term "object side (or image side) of a lens" is defined as the specific range of imaging light rays that pass through the lens surface. The determination of the surface shape of the lens can be performed by the judgment method of a person skilled in the art, i.e., by the sign of the curvature radius (abbreviated as R value). The R value may be commonly used in optical design software, such as Zemax or CodeV. The R value is also commonly found in lens data sheets (lens data sheets) of optical design software. When the R value is positive, the object side is judged to be a convex surface; and when the R value is negative, judging that the object side surface is a concave surface. On the contrary, regarding the image side surface, when the R value is positive, the image side surface is judged to be a concave surface; when the R value is negative, the image side surface is judged to be convex.

The utility model provides a photographic optical lens, which comprises a first lens, a second lens, a third lens, a diaphragm, a fourth lens, a fifth lens and a sixth lens from an object side to an image side in sequence;

the sixth lens is a plastic aspheric surface, and the focal length is positive.

Preferably, the first lens is a convex-concave glass spherical lens with a negative focal length, denoted f1, and a high refractive index material nd >1.8 is used to satisfy the positive f-theta distortion requirement. Meanwhile, 9.5mm < R1<11mm.2.75mm < R2<2.95mm, R1 is the first surface radius of curvature of the first lens. R2 is the second radius of curvature of the second lens.

More preferably, the second lens is a plastic aspherical surface, and the focal length is negative f 2. The requirement of positive f-theta distortion is met in a near step, meanwhile, the edge image effect is required to be good, the second lens adopts a plastic aspheric surface, edge light distribution can be corrected by the plastic aspheric surface, the positive f-theta distortion effect is achieved, and the MTF image quality of the edge is improved. 1.51< nd2<1.57.nd2 is the second lens refractive index.

The third lens element is a biconvex glass sphere with a positive focal length, denoted f 3.

The fourth and fifth lenses are cemented lenses, the fourth lens is a convex-concave negative lens, the fifth lens is a biconvex positive lens, and the focal length after cementing is positive, which is denoted by f 45.

The sixth lens element is a plastic aspherical surface and has a positive focal length, f 6. The position away from the image space uses a plastic aspheric surface, so that aberration can be further corrected, and the image quality effect is improved.

The structure uses an imaging system consisting of six lenses, and a diaphragm is arranged between the third lens and the fourth lens; the focal length of the system is recorded as f, and the focal length ratio of the system to the focal length of the system satisfies the following conditions: 2< | f2/f | <3, 3< | f3/f | <4, 4.5< | f45/f | <6, 5< | f6/f | < 6.

The glass-plastic mixing system is designed by considering the athermalization design, the lens matching support seat is assembled on the module, and the whole system is considered to be athermalized, namely the lens cannot be burnt even when being used in the environment of minus 40 ℃ to 105 ℃, and the imaging is clear in the temperature range. Because the refractive index of the plastic aspheric surface is larger than that of the glass due to temperature change, the third lens and the sixth lens have focal lengths meeting the following conditions in order to meet the athermalization condition: 0.37< | f2/f6| < 0.55.

The lens of the optical system is supported by using an aluminum space ring to match with a metal lens frame, the back focus change is recorded with delta BFL1 at high temperature, the lens uses a metal aluminum supporting seat, and the back focus change is recorded with delta BFL2 and delta BFL 1-delta BFL2 are close to 0 due to the high temperature of the supporting seat. The high temperature of the lens makes the back focus change and the high temperature of the supporting seat makes the back focus change compensate each other, thereby keeping the imaging position unchanged and achieving the purpose of no high temperature defocusing. Similarly, the low temperature condition can also meet the condition that the delta BFL 1-delta BFL2 is close to 0. The optical system structure can avoid the problem of field curvature at the edge due to high and low temperature.

The optical imaging lens of the present invention will be described in detail with reference to specific embodiments.

To further facilitate the description of the present invention, in the imaging lens system, the relationship between the important parameters is defined as follows:

t1 is the central thickness of the first lens on the optical axis; t2 is the central thickness of the second lens on the optical axis; t3 is the central thickness of the third lens on the optical axis; t45 is the sum of the central thicknesses of the fourth and fifth lenses on the optical axis; t6 is the central thickness of the sixth lens on the optical axis; g12 is an air gap on the optical axis from the first lens to the second lens; g23 is an air gap on the optical axis from the second lens to the third lens; g67 is an air gap on the optical axis between the sixth lens and the seventh lens; gstop is the air gap before and after the diaphragm; ALT is the sum of the thicknesses of the lenses of the group on the optical axis; ALG is the system air gap sum; TTL is the distance on the optical axis from the first lens to the imaging surface.

The second lens and the sixth lens of the group of lenses are glass aspheric surfaces.

The equation of the aspheric curve is as follows:

wherein: z: depth of the aspheric surface (the vertical distance between a point on the aspheric surface that is y from the optical axis and a tangent plane tangent to the vertex on the optical axis of the aspheric surface); c: the curvature of the aspheric vertex (the vertex curvature); k: cone coefficient (Conic Constant);

radial distance (radial d)istance)；r_n: normalized radius (normalysis radius (NRADIUS)); u: r/r_n；a_m: mth order Q^conA coefficient; q_m ^con: mth order Q^conA polynomial (the mth Qcon polymonal).

Implement one

As shown in fig. 1, an imaging optical lens includes, in order from an object side to an image side, a first lens element 1, a second lens element 2, a third lens element 3, a stop 4, a fourth lens element 5, a fifth lens element 6, and a sixth lens element 7;

the first lens 1 is a convex-concave glass spherical lens, and the focal length is negative and is marked as f 1;

the second lens 2 is a plastic aspheric surface, and the focal length is negative and is marked as f 2;

the third lens 3 is a biconvex glass spherical surface, and the focal length is positive and is marked as f 3;

the fourth lens 5/6 and the fifth lens 5/6 are cemented lenses, the fourth lens 5 is a convex-concave negative lens, the fifth lens 6 is a biconvex positive lens, and the focal length after cementing is positive and is marked as f 45;

the sixth lens element 7 is an aspherical plastic surface, and has a positive focal length f 6.

In the lens assembly according to the first embodiment, the focal length f is 0.953mm, the aperture value FNO is 2, the image plane Φ 3.96mm, and the field angle FOV is 200 °.

The detailed optical data of this example is shown in Table 1-1.

Tables 1-2 show the aspherical coefficient data in the first example.

Surface of	3	4	11	12
					K＝	-6.3877E+01	1.9368E-01	-8.3059E+01	-5.0976E-01
a4＝	4.3309E-02	1.4845E-01	-1.8343E-02	1.9553E-03
					a6＝	-1.6973E-02	-8.1577E-02	1.0656E-02	-1.1624E-02
a8＝	3.9327E-03	3.1331E-02	-6.5558E-03	1.1590E-02
					a10＝	-5.5210E-04	-7.3777E-03	5.1413E-03	-4.8741E-03
a12＝	3.6674E-05	-1.6359E-03	-1.9077E-03	1.2114E-03
					a14＝	9.8335E-08	1.2348E-03	4.9683E-04	-9.1277E-05
a15＝	-1.0062E-07	-2.0537E-04	-5.8884E-05	1.3765E-05

Tables 1-3 show the focal length ratios of the first embodiment.

f2/f	f3/f	f45/f	f6/f	f2/f6
					-2.39	3.73	5.29	5.20	-0.46

2-5, wherein fig. 2 is a defocus graph in the first embodiment, the horizontal axis is focus shift, the peak is at the focal distance, and the imaging quality is reduced but still high as the focus shift changes; FIG. 3 is a graph of distortion of the first embodiment, in which it can be seen that the distortion reaches more than 18%, and in the same unit field angle, the edge distribution pixels are more than the center, and the edge object is highlighted; fig. 4 is a vertical axis aberration diagram of the first embodiment, and fig. 5 is a lateral chromatic aberration diagram of the first embodiment of the present invention, which shows that the field aberration is small and the color reproducibility is good.

Example two

In all embodiments, the optical structure diagram is identical, with the difference being in the choice of parameters. Due to the differences in the parameter selection, the resulting effects are also significantly different.

In the lens group according to example two, the focal length f is 0.954mm, the aperture value FNO is 2, the image plane Φ 3.93mm, and the FOV is 200 °.

The detailed optical data of this example is shown in Table 2-1.

Table 2-2 shows the aspherical coefficient data in example II.

Surface of	3	4	11	12
					K＝	-4.9103E+01	3.5517E-01	3.2585E+01	-2.0450E+00
A4＝	3.7600E-02	1.5356E-01	-1.9123E-02	8.3349E-03
					A6＝	-1.6498E-02	-9.4714E-02	1.6216E-02	-1.4918E-02
A8＝	3.9629E-03	3.1401E-02	-7.9413E-03	1.8652E-02
					A10＝	-5.4769E-04	-6.3700E-03	5.6802E-03	-7.4441E-03
A12＝	3.4900E-05	-1.2754E-03	-2.2360E-03	1.1721E-03
					A14＝	1.9996E-07	1.2294E-03	6.7147E-04	1.7064E-04
A15＝	-1.0051E-07	-3.1836E-04	-9.4572E-05	-1.0625E-05

Tables 2-3 show the focal length ratios of the second embodiment.

f2/f	f3/f	f45/f	f6/f	f2/f6
					-2.25	3.84	4.89	5.34	-0.42

The detailed explanation of the present embodiment refers to fig. 6-9, in which fig. 6 is a defocus graph in the second embodiment, the horizontal axis is the focal distance, the peak is at the focal distance, and the imaging quality is reduced with the change of the focal distance, but the imaging quality is still high; FIG. 7 is a graph of distortion of the second embodiment, in which it can be seen that the distortion reaches more than 18%, and in the same unit field angle, the edge distribution pixels are more than the center, and the edge object is highlighted; fig. 8 is a vertical axis aberration diagram of the second embodiment, and fig. 9 is a lateral chromatic aberration diagram of the second embodiment of the present invention, it can be seen that the field aberration is small and the color reproducibility is good.

EXAMPLE III

Similarly, in all embodiments, the optical structure diagram is identical, with the difference being in the choice of parameters. Due to the differences in the parameter selection, the resulting effects are also significantly different.

In the lens group according to example three, the focal length f is 0.957mm, the aperture value FNO is 2, the image plane Φ 3.85mm, and the FOV is 200 °.

The detailed optical data of this example is shown in Table 3-1.

Table 3-2 shows the aspherical coefficient data in example III.

Tables 3-3 show the focal length ratios of the third example.

f2/f	f3/f	f45/f	f6/f	f2/f6
					-2.33	3.65	4.97	5.64	-0.41

The detailed explanation of the present embodiment refers to fig. 10-13, in which fig. 10 is a defocus graph in the third embodiment, the horizontal axis is the focal distance, the peak is at the focal distance, and the imaging quality is reduced with the change of the focal distance, but the imaging quality is still high; FIG. 11 is a graph of distortion of the third embodiment, in which it can be seen that the distortion reaches more than 18%, and in the same unit field angle, the edge distribution pixels are more than the center, and the edge object is highlighted; fig. 12 is a vertical axis aberration diagram of the third embodiment, and fig. 13 is a lateral chromatic aberration diagram of the third embodiment of the present invention, it can be seen that the field aberration is small and the color reproducibility is good.

Example four

In the lens group of example four, the lens focal length f is 0.96mm, the aperture value FNO is 2, the image plane Φ 3.94mm, and the FOV is 200 °.

The detailed optical data of this example is shown in Table 4-1.

Table 4-2 shows the aspherical coefficient data in example four.

Surface of	3	4	11	12
					K＝	-6.15708E+01	2.06557E-01	2.01937E+01	-2.05216E+00
A4＝	3.90287E-02	1.42058E-01	-1.32161E-02	7.83262E-03
					A6＝	-1.60793E-02	-8.48887E-02	9.29241E-03	-1.18663E-02
A8＝	3.76322E-03	3.05543E-02	-4.73576E-03	1.30564E-02
					A10＝	-5.24544E-04	-6.74761E-03	4.60939E-03	-5.07204E-03
A12＝	3.53113E-05	-1.31968E-03	-2.21522E-03	8.30515E-04
					A14＝	-6.25715E-08	1.13963E-03	7.43315E-04	1.25834E-04
A15＝	-8.67949E-08	-2.29791E-04	-1.04971E-04	-1.27461E-05

Tables 4-3 show the focal length ratios of the fourth example.

f2/f	f3/f	f45/f	f6/f	f2/f6
					-2.32	3.65	4.93	5.67	-0.41

The detailed explanation of the present embodiment refers to fig. 14-17, in which fig. 14 is a defocus graph in the fourth embodiment, the horizontal axis is the focal distance, the peak value is at the focal distance, and the imaging quality is reduced with the change of the focal distance, but the imaging quality is still high; FIG. 15 is a graph of distortion of the fourth embodiment, in which it can be seen that the distortion reaches more than 18%, and the edge distribution pixels are more than the center at the same unit field angle, so that the edge object is highlighted; fig. 16 is a vertical axis aberration diagram of the fourth embodiment, and fig. 17 is a lateral chromatic aberration diagram of the first embodiment of the present invention, which shows that the field aberration is small and the color reproducibility is good.

EXAMPLE five

In the lens group of example four, the lens focal length f is 0.97mm, the aperture value FNO is 2, the image plane Φ 4.03mm, and the FOV is 200 °.

The detailed optical data of this example is shown in Table 5-1.

Table 5-2 shows the aspherical coefficient data in example V.

Surface of	3	4	11	12
					K＝	-6.38767E+01	1.93675E-01	-8.30592E+01	-5.09758E-01
A4＝	4.10607E-02	1.40741E-01	-1.73906E-02	1.85377E-03
					A6＝	-1.55298E-02	-7.46423E-02	9.75000E-03	-1.06359E-02
A8＝	3.47274E-03	2.76666E-02	-5.78908E-03	1.02346E-02
					A10＝	-4.70509E-04	-6.28738E-03	4.38152E-03	-4.15381E-03
A12＝	3.01629E-05	-1.34545E-03	-1.56906E-03	9.96322E-04
					A14＝	7.80534E-08	9.80092E-04	3.94361E-04	-7.24517E-05
A15＝	-7.70753E-08	-1.57318E-04	-4.51076E-05	1.05446E-05

Tables 4-3 show the focal length ratios of the fourth example.

f2/f	f3/f	f45/f	f6/f	f2/f6
					-2.39	3.74	5.29	5.20	-0.46

The detailed explanation of the present embodiment refers to fig. 18-21, in which fig. 18 is a defocus graph in the fifth embodiment, the horizontal axis is the focal distance, the peak value is at the focal distance, the imaging quality is reduced with the change of the focal distance, but the imaging quality is still high; FIG. 19 is a graph of distortion of the fifth embodiment, in which it can be seen that the distortion reaches more than 18%, and the edge distribution pixels are more than the center at the same unit field angle, so that the edge object is highlighted; fig. 20 is a vertical axis aberration diagram of the fifth embodiment, and fig. 21 is a lateral chromatic aberration diagram of the fifth embodiment of the present invention, it can be seen that the field aberration is small and the color reproducibility is good.

Contrast the embodiment of the utility model provides a first to embodiment five, can find when the parameter changes, imaging characteristic also has some slight differences, but on the whole, when using the camera optical lens of 4G2P structure, no matter high low temperature, as long as the center can not produce the out of focus condition, just can satisfy the problem that the edge can not produce the field curvature.

While the invention has been particularly shown and described with reference to a preferred embodiment, it will be understood by those skilled in the art that various changes in form and detail may be made therein without departing from the spirit and scope of the invention as defined by the appended claims.

Claims

1. An optical lens for image pickup, comprising, in order from an object side to an image side, a first lens element, a second lens element, a third lens element, a diaphragm, a fourth lens element, a fifth lens element and a sixth lens element;

the sixth lens is a plastic aspheric surface, and the focal length is positive.

2. An imaging optical lens according to claim 1, characterized in that it further satisfies: 2< | f2/f | <3, and 3< | f3/f | <4, where f is the system focal length, f2 is the focal length of the second lens, and f3 is the focal length of the third lens.

3. An imaging optical lens according to claim 1, characterized in that it further satisfies: 4.5< | f45/f | <6, and 5< | f6/f | <6, where f is the focal length of the system, f45 is the focal length of the fourth lens cemented with the fifth lens, and f6 is the focal length of the sixth lens.

4. An imaging optical lens according to claim 1, characterized in that it further satisfies: 0.37< | f2/f6| < 0.55.

5. An image pick-up optical lens as claimed in claim 1, characterized in that an aluminum spacer is used between the optics to match the metal frame and a metal aluminum support is used for each lens.

6. An imaging optical lens according to claim 5, wherein the lens high temperature causes the back focus to change as Δ BFL1, and the metallic aluminum support causes the back focus to change as Δ BFL2, Δ BFL1- Δ BFL2 being close to 0.