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CN112285881A - Two-lens small-diameter large-field-angle lens - Google Patents

Two-lens small-diameter large-field-angle lens Download PDF

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Publication number
CN112285881A
CN112285881A CN202010747002.2A CN202010747002A CN112285881A CN 112285881 A CN112285881 A CN 112285881A CN 202010747002 A CN202010747002 A CN 202010747002A CN 112285881 A CN112285881 A CN 112285881A
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lens
field
image side
lenses
stop
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陈俊宏
张若金
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Hubei Huaxin Photoelectric Co ltd
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Hubei Huaxin Photoelectric Co ltd
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Priority to CN202010747002.2A priority Critical patent/CN112285881A/en
Publication of CN112285881A publication Critical patent/CN112285881A/en
Priority to PCT/CN2021/099857 priority patent/WO2022022116A1/en
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    • GPHYSICS
    • G02OPTICS
    • G02BOPTICAL ELEMENTS, SYSTEMS OR APPARATUS
    • G02B13/00Optical objectives specially designed for the purposes specified below
    • G02B13/001Miniaturised objectives for electronic devices, e.g. portable telephones, webcams, PDAs, small digital cameras
    • G02B13/0015Miniaturised objectives for electronic devices, e.g. portable telephones, webcams, PDAs, small digital cameras characterised by the lens design
    • G02B13/002Miniaturised objectives for electronic devices, e.g. portable telephones, webcams, PDAs, small digital cameras characterised by the lens design having at least one aspherical surface
    • G02B13/003Miniaturised objectives for electronic devices, e.g. portable telephones, webcams, PDAs, small digital cameras characterised by the lens design having at least one aspherical surface having two lenses
    • GPHYSICS
    • G02OPTICS
    • G02BOPTICAL ELEMENTS, SYSTEMS OR APPARATUS
    • G02B13/00Optical objectives specially designed for the purposes specified below
    • G02B13/001Miniaturised objectives for electronic devices, e.g. portable telephones, webcams, PDAs, small digital cameras
    • G02B13/0015Miniaturised objectives for electronic devices, e.g. portable telephones, webcams, PDAs, small digital cameras characterised by the lens design
    • G02B13/005Miniaturised objectives for electronic devices, e.g. portable telephones, webcams, PDAs, small digital cameras characterised by the lens design having spherical lenses only
    • GPHYSICS
    • G02OPTICS
    • G02BOPTICAL ELEMENTS, SYSTEMS OR APPARATUS
    • G02B13/00Optical objectives specially designed for the purposes specified below
    • G02B13/06Panoramic objectives; So-called "sky lenses" including panoramic objectives having reflecting surfaces

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  • General Physics & Mathematics (AREA)
  • Optics & Photonics (AREA)
  • Lenses (AREA)

Abstract

本发明公开了一种两镜片小直径大视场角的镜头,其特征在于,从物方开始,沿光轴到像方,依次设置有:第一透镜L1、孔径光阑Stop以及第二透镜L2;其中,所述第一透镜L1为负透镜,其具有第一表面和中央位置凹向像方的第二表面;所述第二透镜L2为正透镜,其具有第三表面和凸向像方的第四表面;所述孔径光阑Stop位于第一透镜L1和第二透镜L2之间,用于平衡两镜片的外径大小。本发明采用两片镜片,能够在狭小空间拍摄,满足镜头外径小的尺寸要求和大视场角的功能,可以用在拍摄空间狭小或者镜头的安装空间狭小的领域。The invention discloses a lens with two lenses of small diameter and large field of view, which is characterized in that, starting from the object side, along the optical axis to the image side, a first lens L1, an aperture stop Stop and a second lens are sequentially arranged. L2; wherein, the first lens L1 is a negative lens, which has a first surface and a second surface concave to the image side at the center position; the second lens L2 is a positive lens, which has a third surface and a convex image side The fourth surface of the square; the aperture stop Stop is located between the first lens L1 and the second lens L2, and is used to balance the outer diameters of the two lenses. The invention adopts two lenses, can shoot in a narrow space, meets the size requirements of small outer diameter of the lens and the function of large field of view, and can be used in the field where the shooting space is narrow or the installation space of the lens is narrow.

Description

Two-lens small-diameter large-field-angle lens
Technical Field
The invention relates to the technical field of lenses, in particular to a two-lens small-diameter large-field-angle lens.
Background
In some application fields (such as medical science, industry, environmental protection, scientific research, search, exploration and other various fields), a small shooting space or a small installation space of the lens not only needs the outer diameter of the lens to be small, but also needs to satisfy the function of a large field angle.
Therefore, how to provide a two-lens small-diameter large-field-angle lens that can satisfy the above requirements is a problem that needs to be solved by those skilled in the art.
Disclosure of Invention
In view of the above, the present invention provides a two-lens small-diameter large-field-angle lens, which can not only capture images in a narrow space, but also satisfy the requirements of small outer diameter and large field angle.
In order to achieve the purpose, the invention provides the following technical scheme:
the lens with two lenses, small diameter and large field angle is characterized in that the lens is sequentially provided with the following components from an object side to an image side along an optical axis: a first lens (L1), an aperture Stop (Stop), and a second lens (L2); wherein the first lens (L1) is a negative lens having a first surface and a second surface whose central position is concave to the image side; the second lens (L2) is a positive lens having a third surface and a fourth surface convex to the image side; the aperture Stop (Stop) is positioned between the first lens (L1) and the second lens (L2) and is used for balancing the outer diameter of the two lenses.
Preferably, in the above two-lens small-diameter large-field-angle lens, the surfaces of the first lens (L1) and the second lens (L2) are spherical or aspherical.
Preferably, in the two-lens small-diameter large-angle lens described above, an optical filter (IR) is provided on the image side of the second lens (L2).
Preferably, in the above two-lens small-diameter large-field-angle lens, the lens satisfies the following conditions: 0.1< (Tfs/f)/tan (hfov) < 0.5; wherein, Tfs is: the distance from the center of the object space surface of the first lens (L1) to the aperture Stop (Stop); f is the effective focal length of the lens; the HFOV is half of the maximum field angle.
Preferably, in the above two-lens small-diameter large-field-angle lens, the lens satisfies the following conditions: 1< f/f2< 2; wherein f is the effective focal length of the lens; f2 is the focal length of the second lens.
Preferably, in the above two-lens small-diameter large-field-angle lens, the lens satisfies the following conditions: 0.1< [ Ho/tan (HFOV) ]/f < 0.5; the Ho is the height of the light at the edge of the object space surface of the first lens when the maximum field angle is achieved; HFOV is half of the maximum field angle; f is the effective focal length of the lens.
According to the technical scheme, compared with the prior art, the invention has the following characteristics:
a first lens (L1) which is a negative lens and is beneficial to realizing a large field angle;
the aperture diaphragm (Stop) is positioned between the two lenses, and the outer diameters of the two lenses are balanced, so that the requirement of small outer diameter of the lens is favorably met;
the second lens (L2) is a positive lens, and the focal power required by the lens for imaging is mainly provided by the second lens;
the invention adopts two lenses, can shoot in narrow space, meets the size requirement of small outer diameter of the lens and the function of large field angle, and can be used in the field of narrow shooting space or narrow installation space of the lens.
Drawings
In order to more clearly illustrate the embodiments of the present invention or the technical solutions in the prior art, the drawings used in the description of the embodiments or the prior art will be briefly described below, it is obvious that the drawings in the following description are only embodiments of the present invention, and for those skilled in the art, other drawings can be obtained according to the provided drawings without creative efforts.
FIG. 1 is a schematic diagram of the present invention.
Fig. 2 is a schematic structural diagram of embodiment 1 of the present invention.
FIG. 3 is a light ray fan diagram of embodiment 1 of the present invention.
FIG. 4 is a graph showing curvature of field and distortion in example 1 of the present invention.
Fig. 5 is a graph showing MTF resolution in embodiment 1 of the present invention.
Fig. 6 is a schematic structural diagram of embodiment 2 of the present invention.
FIG. 7 is a light ray fan diagram according to example 2 of the present invention.
Fig. 8 is a graph showing curvature of field and distortion in example 2 of the present invention.
Fig. 9 is a graph showing MTF resolution in embodiment 2 of the present invention.
Fig. 10 is a schematic structural diagram of embodiment 3 of the present invention.
FIG. 11 is a light ray fan diagram of embodiment 3 of the present invention.
FIG. 12 is a graph showing curvature of field and distortion in example 3 of the present invention.
FIG. 13 is a graph showing MTF resolution in embodiment 3 of the present invention
FIG. 14 is a schematic structural diagram of embodiment 4 of the present invention.
Figure 15 is a ray fan diagram of embodiment 4 of the present invention.
FIG. 16 is a graph showing curvature of field and distortion in example 4 of the present invention.
FIG. 17 is a graph showing MTF resolution in embodiment 4 of the present invention.
Detailed Description
The technical solutions in the embodiments of the present invention will be clearly and completely described below with reference to the drawings in the embodiments of the present invention, and it is obvious that the described embodiments are only a part of the embodiments of the present invention, and not all of the embodiments. All other embodiments, which can be derived by a person skilled in the art from the embodiments given herein without making any creative effort, shall fall within the protection scope of the present invention.
Example 1: fig. 2 is a schematic view of an optical lens according to a first embodiment of the invention. As shown in fig. 2 to 5, the first lens L1, the aperture Stop, the second lens L2, the optical filter (IR), and the Image plane Image are disposed in this order from the object side to the Image side along the optical axis according to the first embodiment of the present invention; a first lens L1 having a first surface S1 and a second surface S2 whose central position is concave to the image side; the aperture Stop has a surface S3; a second lens L2 having a third surface S4 and a fourth surface S5 convex to the image side; the filter IR has a first surface S6 facing the object side and a second surface S7 facing the image side; the Image plane Image has a surface S8.
Lens data of the above-described lens are shown in tables 1 and 2 below.
[ TABLE 1 ]
Figure BDA0002608715220000041
[ TABLE 2 ]
Figure BDA0002608715220000042
Figure BDA0002608715220000051
The conditions satisfied by the above-described lens are shown in table 3.
[ TABLE 3 ]
Marking Content of the presentation Numerical value
f Effective focal length of lens 1.469
HFOV Half of maximum field angle 70
f1 Focal length of the first lens (L1) -1.638
f2 Focal point of the second lens (L2)Distance between 1.17
Ho The first lens (L1) object side surface edge ray height at maximum field angle. 0.782
Tfs The distance from the center of the object space surface of the first lens (L1) to the aperture Stop (Stop) 0.907
2、 0.1<(Tfs/f)/tan(HFOV)<0.5 0.225
3、 1<f/f2<2 1.256
4、 0.1<[Ho/tan(HFOV)]/f<0.5 0.194
In the above embodiment:
as shown in fig. 3 (light sector), it can be seen that the spherical aberration of the lower order has been corrected well and the spherical aberration of the higher order is smaller.
As shown in fig. 4 (field curvature and distortion diagram), the distortion curve is relatively smooth, which effectively improves the definition of the expanded image.
As shown in fig. 5 (MTF resolution graph), it can be seen from the curves that MTF curves of the meridian and the sagittal of each field of view are relatively close, which indicates that the lens has relatively good imaging consistency in both directions of the meridian (T) and the sagittal (S), and the lens has relatively good imaging effect and resolution.
Example 2:
fig. 5 is a schematic view of an optical lens according to a second embodiment of the present invention. As shown in fig. 6 to 9, the first lens L1, the aperture Stop, the second lens L2, the optical filter (IR), and the Image plane Image are disposed in this order from the object side to the Image side along the optical axis according to the second embodiment of the present invention; a first lens L1 having a first surface S1 and a second surface S2 whose central position is concave to the image side; the aperture Stop has a surface S3; a second lens L2 having a third surface S4 and a fourth surface S5 convex to the image side; the filter IR has a first surface S6 facing the object side and a second surface S7 facing the image side; the Image plane Image has a surface S8.
Lens data of the above lenses are shown in table 4 below.
[ TABLE 4 ]
Figure BDA0002608715220000061
The conditions satisfied by the above-described lens are shown in table 5.
[ TABLE 5 ]
Marking Content of the presentation Numerical value
f Effective focal length of lens 1.008
HFOV Half of maximum field angle 60
f1 Focal length of the first lens (L1) -2.27
f2 Focal length of the second lens (L2) 0.806
Ho The first lens (L1) object side surface edge ray height at maximum field angle. 0.392
Tfs The distance from the center of the object space surface of the first lens (L1) to the aperture Stop (Stop) 0.365
2、 0.1<(Tfs/f)/tan(HFOV)<0.5 0.209
3、 1<f/f2<2 1.251
4、 0.1<[Ho/tan(HFOV)]/f<0.5 0.225
In the above embodiment:
as shown in fig. 7 (light sector), it can be seen that the spherical aberration of the lower order has been corrected well and the spherical aberration of the higher order is smaller.
As shown in fig. 8 (field curvature and distortion diagram), the distortion curve is relatively smooth, which effectively improves the definition of the expanded image.
As shown in fig. 9 (MTF resolution graph), it can be seen from the curves that MTF curves of the meridian and the sagittal of each field of view are relatively close, which indicates that the lens has relatively good imaging consistency in both directions of the meridian (T) and the sagittal (S), and the lens has relatively good imaging effect and resolution.
Example 3:
fig. 10 is a schematic view of an optical lens according to a third embodiment of the present invention. As shown in fig. 10 to 13, the first lens L1, the aperture Stop, the second lens L2, the filter IR, and the Image plane Image are disposed in this order from the object side to the Image side along the optical axis according to the third embodiment of the present invention; a first lens L1 having a first surface S1 and a second surface S2 whose central position is concave to the image side; the aperture Stop has a surface S3; a second lens L2 having a third surface S4 and a fourth surface S5 convex to the image side; the filter IR has a first surface S6 facing the object side and a second surface S7 facing the image side; the Image plane Image has a surface S8.
Lens data of the above lenses are shown in table 6 below.
[ TABLE 6 ]
Figure BDA0002608715220000081
The conditions satisfied by the above-described lens are shown in table 7.
[ TABLE 7 ]
Marking Content of the presentation Numerical value
f Effective focal length of lens 1.037
HFOV Half of maximum field angle 60
f1 Focal length of the first lens (L1) -2.093
f2 Focal length of the second lens (L2) 0.825
Ho The first lens (L1) object side surface edge ray height at maximum field angle. 0.365
Tfs A first lens (L1) object spaceDistance from surface center to aperture Stop (Stop) 0.359
2、 0.1<(Tfs/f)/tan(HFOV)<0.5 0.200
3、 1<f/f2<2 1.257
4、 0.1<[Ho/tan(HFOV)]/f<0.5 0.203
In the above embodiment:
as shown in fig. 11 (light sector), it can be seen that the spherical aberration of the lower order has been corrected well and the spherical aberration of the higher order is smaller.
As shown in fig. 12 (field curvature and distortion diagram), the distortion curve is relatively smooth, and the definition of the expanded image is effectively improved.
As shown in fig. 13 (MTF resolution graph), it can be seen from the curves that MTF curves of the meridian and the sagittal of each field of view are relatively close, which indicates that the lens has relatively good imaging consistency in both directions of the meridian (T) and the sagittal (S), and the lens has relatively good imaging effect and resolution.
Example 4:
fig. 14 is a schematic view of an optical lens according to a fourth embodiment of the invention. As shown in fig. 14 to 17, the first lens L1, the aperture Stop, the second lens L2, the filter IR, and the Image plane Image are disposed in this order from the object side to the Image side along the optical axis according to the fourth embodiment of the present invention; a first lens L1 having a surface S1 and a second surface S2 whose central position is concave to the image side; the aperture Stop has a surface S3; a second lens L2 having a third surface S4 and a fourth surface S5 convex to the image side; the filter IR has a first surface S6 facing the object side and a second surface S7 facing the image side; the Image plane Image has a surface S8.
Lens data of the above lenses are shown in table 8 below.
[ TABLE 8 ]
Figure BDA0002608715220000091
The conditions satisfied by the above-described lens are shown in table 9.
[ TABLE 9 ]
Marking Content of the presentation Numerical value
f Effective focal length of lens 1.038
HFOV Half of maximum field angle 60
f1 First pass throughFocal length of mirror (L1) -1.994
f2 Focal length of the second lens (L2) 0.813
Ho The first lens (L1) object side surface edge ray height at maximum field angle. 0.365
Tfs The distance from the center of the object space surface of the first lens (L1) to the aperture Stop (Stop) 0.356
2、 0.1<(Tfs/f)/tan(HFOV)<0.5 0.198
3、 1<f/f2<2 1.277
4、 0.1<[Ho/tan(HFOV)]/f<0.5 0.203
In the above embodiment:
as shown in fig. 15 (light sector), it can be seen that the spherical aberration of the lower order has been corrected well and the spherical aberration of the higher order is smaller.
As shown in fig. 16 (field curvature and distortion diagram), the distortion curve is relatively smooth, and the definition of the expanded image is effectively improved.
As shown in fig. 17 (MTF resolution graph), it can be seen from the curves that MTF curves of the meridian and the sagittal of each field of view are relatively close, which indicates that the lens has relatively good imaging consistency in both directions of the meridian (T) and the sagittal (S), and the lens has relatively good imaging effect and resolution.
As described above, the two-lens small-diameter large-field-angle lens according to the present invention satisfies both the size requirement for a small outer diameter of the lens and the function of a large field angle, and has a simple structure, and can perform photographing in a narrow space.
The embodiments in the present description are described in a progressive manner, each embodiment focuses on differences from other embodiments, and the same and similar parts among the embodiments are referred to each other. The device disclosed by the embodiment corresponds to the method disclosed by the embodiment, so that the description is simple, and the relevant points can be referred to the method part for description.
The previous description of the disclosed embodiments is provided to enable any person skilled in the art to make or use the present invention. Various modifications to these embodiments will be readily apparent to those skilled in the art, and the generic principles defined herein may be applied to other embodiments without departing from the spirit or scope of the invention. Thus, the present invention is not intended to be limited to the embodiments shown herein but is to be accorded the widest scope consistent with the principles and novel features disclosed herein.

Claims (6)

1.一种两镜片小直径大视场角的镜头,其特征在于,从物方开始,沿光轴到像方,依次设置有:第一透镜(L1)、孔径光阑(Stop)以及第二透镜(L2);其中,所述第一透镜(L1)为负透镜,其具有第一表面和中央位置凹向像方的第二表面;所述第二透镜(L2)为正透镜,其具有第三表面和凸向像方的第四表面;所述孔径光阑(Stop)位于第一透镜(L1)和第二透镜(L2)之间,用于平衡两镜片的外径大小。1. a lens with a small diameter of two lenses and a large field of view, characterized in that, starting from the object side, along the optical axis to the image side, sequentially provided with: a first lens (L1), an aperture stop (Stop) and a first lens Two lenses (L2); wherein, the first lens (L1) is a negative lens, which has a first surface and a second surface whose central position is concave toward the image side; the second lens (L2) is a positive lens, which It has a third surface and a fourth surface convex to the image side; the aperture stop (Stop) is located between the first lens (L1) and the second lens (L2), and is used to balance the outer diameters of the two lenses. 2.根据权利要求1所述的一种两镜片小直径大视场角的镜头,其特征在于,所述第一透镜(L1)和第二透镜(L2)的表面为球面或非球面。2 . The lens with two lenses of small diameter and large field of view according to claim 1 , wherein the surfaces of the first lens ( L1 ) and the second lens ( L2 ) are spherical or aspherical. 3 . 3.根据权利要求1所述的一种两镜片小直径大视场角的镜头,其特征在于,所述第二透镜(L2)的像方一侧设有滤光片(IR)。3 . The lens of claim 1 , wherein the second lens ( L2 ) is provided with a filter (IR) on the image side side. 4 . 4.根据权利要求1所述的一种两镜片小直径大视场角的镜头,其特征在于,该镜头满足下列条件:0.1<(Tfs/f)/tan(HFOV)<0.5;其中,Tfs为:第一透镜(L1)物方表面中心到孔径光阑(Stop)的距离;f为镜头的有效焦距;HFOV为最大视场角的一半。4. The lens of claim 1, wherein the lens satisfies the following conditions: 0.1<(Tfs/f)/tan(HFOV)<0.5; wherein, Tfs is: the distance from the center of the object surface of the first lens (L1) to the aperture stop (Stop); f is the effective focal length of the lens; HFOV is half of the maximum angle of view. 5.根据权利要求4所述的一种两镜片小直径大视场角的镜头,其特征在于,该镜头满足下列条件:1<f/f2<2;其中,f为镜头的有效焦距;f2为第二透镜(L2)的焦距。5. The lens of claim 4, wherein the lens satisfies the following conditions: 1<f/f2<2; wherein, f is the effective focal length of the lens; f2 is the focal length of the second lens (L2). 6.根据权利要求5所述的一种两镜片小直径大视场角的镜头,其特征在于,该镜头满足下列条件:0.1<[Ho/tan(HFOV)]/f<0.5;其中,Ho为最大视场角时第一透镜(L1)物方表面边缘光线高度;HFOV为最大视场角的一半;f为镜头的有效焦距。6 . The lens of claim 5 , wherein the lens satisfies the following conditions: 0.1<[Ho/tan(HFOV)]/f<0.5; wherein, Ho is the height of the edge light on the object surface of the first lens (L1) at the maximum field of view; HFOV is half of the maximum field of view; f is the effective focal length of the lens.
CN202010747002.2A 2020-07-29 2020-07-29 Two-lens small-diameter large-field-angle lens Pending CN112285881A (en)

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CN109196519A (en) * 2018-08-21 2019-01-11 深圳市汇顶科技股份有限公司 Lens system, fingerprint identification device and terminal device
CN212623307U (en) * 2020-07-29 2021-02-26 湖北华鑫光电有限公司 A two-lens lens with small diameter and large field of view

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WO2022022116A1 (en) * 2020-07-29 2022-02-03 湖北华鑫光电有限公司 Two-lens piece small-diameter lens having large field of view

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