CN107367828A - A kind of large aperture 4K tight shots - Google Patents

A kind of large aperture 4K tight shots Download PDF

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Publication number
CN107367828A
CN107367828A CN201710833067.7A CN201710833067A CN107367828A CN 107367828 A CN107367828 A CN 107367828A CN 201710833067 A CN201710833067 A CN 201710833067A CN 107367828 A CN107367828 A CN 107367828A
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lens
concave
power
negative
power lenses
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何剑炜
刘官禄
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Dongguan Yutong Optical Technology Co Ltd
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Dongguan Yutong Optical Technology Co Ltd
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Priority to CN201710833067.7A priority Critical patent/CN107367828A/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
    • G02B13/0045Miniaturised 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 five or more lenses
    • GPHYSICS
    • G02OPTICS
    • G02BOPTICAL ELEMENTS, SYSTEMS OR APPARATUS
    • G02B1/00Optical elements characterised by the material of which they are made; Optical coatings for optical elements
    • GPHYSICS
    • G02OPTICS
    • G02BOPTICAL ELEMENTS, SYSTEMS OR APPARATUS
    • G02B1/00Optical elements characterised by the material of which they are made; Optical coatings for optical elements
    • G02B1/04Optical elements characterised by the material of which they are made; Optical coatings for optical elements made of organic materials, e.g. plastics
    • 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
    • GPHYSICS
    • G02OPTICS
    • G02BOPTICAL ELEMENTS, SYSTEMS OR APPARATUS
    • G02B13/00Optical objectives specially designed for the purposes specified below
    • G02B13/18Optical objectives specially designed for the purposes specified below with lenses having one or more non-spherical faces, e.g. for reducing geometrical aberration

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

Abstract

The present invention provides a kind of large aperture 4K tight shots, including the first lens, the second lens, the 3rd lens, the 4th lens, the 5th lens, the 6th lens, the 7th lens and the 8th lens being arranged in order along optical axis from object space to image space, first lens, the 3rd lens, the 4th lens, the 5th lens and the 8th lens are glass lens, and second lens, the 6th lens and the 7th lens are plastic aspheric lens.The present invention uses 5 sheet glass spherical lenses and 8 optical textures of 3 plastic aspheric lens, visible ray and infrared light can be realized while reach 4K resolution ratio, F1.4 maximum rings, 1/1.8 " the maximum 160 degree angle of visual field of image planes and optics overall length are less than indexs such as 30mm.

Description

A kind of large aperture 4K tight shots
Technical field
The present invention relates to lens technology field, more particularly to a kind of large aperture 4K tight shots.
Background technology
Because article size is different in safety monitoring, far and near difference, and camera lens magnifying power difference are generally required picture Amplify preferably to identify.But the full HD camera pixel of tradition only has 2 mega pixels, if desired by monitored picture amplification then Can be because pixel be relatively low so that details is smudgy after picture amplification.Therefore safety-security area has gradually risen 4K ultra high-definitions in recent years Concept, by very-high solution, 4K security monitoring video cameras even if by picture amplification can also keep higher resolution, be advantageous to more Identify target well.Safety monitoring needs all-weather uninterruptedly to carry out simultaneously, and good picture can not only be presented on daytime micro- It is also required to present clearly bright image under light and night environment.And brightness of image is determined by two factors, one is mirror Head aperture size, one be imaging sensor photoperceptivity.With the photosensitive energy of imaging sensor for current scientific and technological level Power depend on single pixel area, single pixel area it is bigger its by the more good often poor light condition figure below image brightness of light ability more It is high.Therefore there is one kind 1/1.8 " big image planes 4K imaging sensors, be compared at present that common 1/2.5 " 4K images pass It significantly increases single pixel area to sensor, possesses preferably by light ability.
But it can reach 1/1.8 on the market at present " 4K wide-angle tight shot is also seldom, and some extraordinary camera lenses perhaps can be with Reaching 1/1.8, " still often price is too high or does not possess infrared confocal ability for 4K index.Therefore a large aperture is developed 1/1.8 " 4K wide-angle tight shot just seems necessary.For traditional glass spheric glass, it corrects aberration It is limited in one's ability, while price is higher.If desired a 4K ultra high-definitions are designed, the wide-angle tight shot of large aperture then needs more Eyeglass, undoubtedly the production cost of camera lens is greatly improved, be unfavorable for marketing.
The content of the invention
The present invention provides a kind of large aperture 4K tight shots, overcomes the technical problem of Shortcomings in the prior art.
In order to solve the above-mentioned technical problem, the technical solution used in the present invention is:
A kind of large aperture 4K tight shots, including the first lens, second saturating being arranged in order along optical axis from object space to image space Mirror, the 3rd lens, the 4th lens, the 5th lens, the 6th lens, the 7th lens and the 8th lens, it is first lens, the 3rd saturating Mirror, the 4th lens, the 5th lens and the 8th lens are glass lens, and second lens, the 6th lens and the 7th lens are modeling Expect non-spherical lens.
Further, second lens, the 6th lens and the 7th lens meet following conditional with whole camera lens respectively:
2<∣f2/f∣<6;
0.8<∣f6/f∣<4;
0.8<∣f7/f∣<5;
0.4<∣f6/f7∣<4.5;
Wherein, f is the focal length of whole camera lens, and f2, f6 and f7 correspond to the second lens, the 6th lens and the 7th lens respectively Focal length.
Further, the 4th lens and the 5th lens are glued forms balsaming lens, the balsaming lens with it is whole Camera lens meets following conditional:
3.5<∣fe/f∣<80, wherein, fe is the focal length of balsaming lens.
Preferably, first lens are convex-concave negative-power lenses, and second lens are concavo-convex negative-power lenses, 3rd lens are convex flat positive power lens, and the 4th lens are biconvex positive power lens, and the 5th lens are Concave-concave negative-power lenses, the 6th lens are biconvex positive power lens, and the 7th lens are concave-concave negative-power lenses, and the 8th is saturating Mirror is biconvex positive power lens.
Preferably, first lens are convex-concave negative-power lenses, and second lens are concavo-convex negative-power lenses, 3rd lens are biconvex positive power lens, and the 4th lens are biconvex positive power lens, and the 5th lens are Concave-concave negative-power lenses, the 6th lens are biconvex positive power lens, and the 7th lens are that concave-concave negative power is saturating Mirror, the 8th lens are biconvex positive power lens.
Preferably, first lens are convex-concave negative-power lenses, and second lens are concavo-convex negative-power lenses, 3rd lens are biconvex positive power lens, and the 4th lens are biconvex positive power lens, and the 5th lens are Concave-concave negative-power lenses, the 6th lens are biconvex positive power lens, and the 7th lens are that concave-concave negative power is saturating Mirror, the 8th lens are convex-concave positive power lens.
The present invention provides a kind of large aperture 4K tight shots, including is arranged in order along optical axis from object space to image space first saturating Mirror, the second lens, the 3rd lens, the 4th lens, the 5th lens, the 6th lens, the 7th lens and the 8th lens, its feature exist In:First lens, the 3rd lens, the 4th lens, the 5th lens and the 8th lens are glass lens, second lens, 6th lens and the 7th lens are plastic aspheric lens.
It is aspherical that there is higher correction aberration ability, it usually can reduce eyeglass number using the camera lens of aspherical lens Amount, simplify lens construction.Plastic aspherical element eyeglass possesses the ability of good correction aberration, while price is relatively low.Using plastics The mode that aspherical lens mix with glass lens come manufacture and design camera lens can obtain imaging image quality it is outstanding, price is relatively reasonable Product.By the present invention in that combine to form 8 chip optical textures with 5 sheet glass spherical lenses and 3 plastic aspheric lens, And the relative position of the suitable lens of reasonable selection and layout lens, visible ray and infrared light can be realized while reach 4K resolutions Rate, F1.4 maximum ring, 1/1.8 " the maximum 160 degree angle of visual field of image planes and optics overall length less than indexs such as 30mm, and Cost is relatively low, market prospects are extensive.
Brief description of the drawings
Fig. 1 is a kind of first embodiment structural representation of large aperture 4K tight shots of the present invention;
Fig. 2 is a kind of second embodiment structural representation of large aperture 4K tight shots of the present invention;
Fig. 3 is a kind of 3rd embodiment structural representation of large aperture 4K tight shots of the present invention.
Embodiment
Below in conjunction with the accompanying drawings, embodiments of the present invention are specifically illustrated, accompanying drawing is only for reference and explanation uses, and does not form pair The limitation of scope of patent protection of the present invention.
As shown in Figures 1 to 3, a kind of large aperture 4K tight shots, including be arranged in order along optical axis from object space to image space One lens 1, the second lens 2, the 3rd lens 3, the 4th lens 4, the 5th lens 5, the 6th lens 6, the 7th lens 7 and the 8th lens 8, first lens 1, the 3rd lens 3, the 4th lens 4, the 5th lens 5 and the 8th lens 8 are glass lens, and described second is saturating Mirror 2, the 6th lens 6 and the 7th lens 7 are plastic aspheric lens.
Further, second lens 2, the 6th lens 6 and the 7th lens 7 meet following condition with whole camera lens respectively Formula:
2<∣f2/f∣<6;
0.8<∣f6/f∣<4;
0.8<∣f7/f∣<5;
0.4<∣f6/f7∣<4.5;
Wherein, f is the focal length of whole camera lens, and f2, f6 and f7 correspond to the second lens, the 6th lens and the 7th lens respectively Focal length.
Further, the 4th lens 4 and the 5th lens 5 are glued forms balsaming lens, the balsaming lens with it is whole Individual camera lens meets following conditional:3.5<∣fe/f∣<80, wherein, fe is the focal length of balsaming lens.
Embodiment one:Fig. 1 is refer to, first lens 1 are convex-concave negative-power lenses, and second lens 2 are recessed Convex negative-power lenses, the 3rd lens 3 are convex flat positive power lens, and the 4th lens 4 are that biconvex positive light coke is saturating Mirror, the 5th lens 5 are concave-concave negative-power lenses, and the 6th lens 6 are biconvex positive power lens, and the 7th lens 7 are double Recessed negative-power lenses, the 8th lens 8 are biconvex positive power lens.
First lens are as shown in the table to the 8th lens parameters:
F1=-13.5~-4.5 N1=1.43~1.85 R1=15~500 R2=3.1~6.1
F2=-31.5~-10.1 N2=1.47~1.68 R3=-8.9~-3.1 R4=-50~-4.5
F3=6.5~20.5 N3=1.7~2.1 R5=5~50 R6=PL
F4=3.3~15.5 N4=1.43~1.7 R7=5.5~19.7 R8=-9.2~-3
F5=-13.5~-3.2 N5=1.43~1.8 R9=-9.2~-3 R10=5~50
F6=5.1~18.3 N6=1.46~1.65 R11=5.6~19.2 R12=-4.5~-18.5
F7=-25.3~-7.1 N7=1.5~1.75 R13=-25.3~-9.6 R14=9.6~30.2
F8=6.5~22.1 N8=1.43~1.7 R15=5.3~21.5 R16=- ∞~-15
Wherein, f1 to f8 represents the first lens to the focal length of lens of the 8th lens respectively in order;N1 to n8 is in order The first lens are represented respectively to the refractive index of the 8th lens;R1, R3, R5, R7, R9, R11, R13, R15 are represented respectively in order Radius of curvature of first lens to the 8th lens towards object space side centre of surface, R2, R4, R6, R8, R10, R12, R14, R16 represents radius of curvature of first lens to the 8th lens towards image space side centre of surface, the "-" side of representative respectively in order To be negative.
Because the second lens, the 6th lens and the 7th lens are non-spherical lens, each lens mirror shape expires for its Sufficient following equation:
Wherein, r represents radial coordinate, and unit is identical with length of lens unit, and c is the song corresponding to surface central radius Rate, k are circular cone whose conic coefficient, α1To α8For high order aspheric surface coefficient.
Meet that the asphericity coefficient of above-mentioned aspherical equation formula is as shown in the table in embodiment one:
In the present embodiment, the optical physics parameter of the first lens to the 8th lens is as shown in the table:
Face sequence number Face type R D nd K values
S1 Sphere 33.13 0.55 1.63
S2 Sphere 4.502 4.05
S3 It is aspherical -4.671 3 1.66 -0.535
S4 It is aspherical -8.911 0.1 -1.293
S5 Sphere 10.645 1.7 1.95
S6 Sphere PL 0
Diaphragm Plane PL 4.4
S7 Sphere 8.014 3.6 1.43
S8 Sphere -5.211
S9 Sphere -5.211 0.6 1.65
S10 Sphere 27.43 0.1
S11 It is aspherical 11.121 1.75 1.55 0.335
S12 It is aspherical -8.571 0.05 -19.553
S13 It is aspherical -16.533 0.93 1.65 -6.101
S14 It is aspherical 21.55 0.1 -30.572
S15 Sphere 8.573 1.97 1.6
S16 Sphere -220.23
Wherein, R is surface central radius size, and D is to correspond to optical surface to next optical surface in the distance on optical axis; Nd corresponds to the refractive index of d light (wavelength 587nm);S1 and S2 is the object side surface and image interface of the first lens 1, and S3 and S4 are The object side surface and image interface of second lens 2, S5 and S6 are the object side surface and image interface of the 3rd lens 3, and diaphragm is light Plane where late;S7 and S8 is the object side surface and image interface of the 4th lens 4;S9 and S10 is the object side surface of the 5th lens 5 And image interface;S11 and S12 is the object side surface and image interface of the 6th lens 6;S13 and S14 is the object space of the 7th lens 7 Surface and image interface;S15 and S16 is the object side surface and image interface of the 8th lens 8.
Embodiment two:Fig. 2 is refer to, compared with embodiment one, the number amount and type of lens are essentially identical, but specifically Lens parameter and layout are different.
First lens 1 are convex-concave negative-power lenses, and second lens 2 are concavo-convex negative-power lenses, described 3rd lens 3 are biconvex positive power lens, and the 4th lens 4 are biconvex positive power lens, and the 5th lens 5 are double Recessed negative-power lenses, the 6th lens 6 are biconvex positive power lens, and the 7th lens 7 are that concave-concave negative power is saturating Mirror, the 8th lens 8 are biconvex positive power lens.
First lens are as shown in the table to the 8th index of refraction in lens, focal length and radius of curvature parameter:
F1=-11.5~-4.5 N1=1.43~1.85 R1=15~200 R2=3.1~8.9
F2=-21.5~-10.1 N2=1.47~1.68 R3=-8.9~-3.1 R4=-40~-4.5
F3=6.5~13.5 N3=1.7~2.1 R5=5~50 R6=-400~-10
F4=6.5~15.5 N4=1.43~1.7 R7=5.5~35 R8=-9.2~-3
F5=-10~-3 N5=1.43~1.8 R9=-9.2~-3 R10=5~80
F6=5.1~12.3 N6=1.46~1.65 R11=5.6~19.2 R12=-18.5~-4.5
F7=-20.3~-7.5 N7=1.5~1.75 R13=-70~-9.6 R14=5~35
F8=10~21 N8=1.43~1.7 R15=5.3~16.5 R16=- ∞~-10
Meet that the asphericity coefficient of above-mentioned aspherical equation formula is as shown in the table in embodiment two:
S3 S4 S11 S12 S13 S14
α1 0 0 0 0 0 0
α2 3.11E-03 6.75E-04 1.48E-03 -2.98E-03 -7.04E-03 -3.16E-03
α3 5.47E-05 1.59E-05 -5.38E-05 3.37E-04 7.78E-04 4.13E-04
α4 -1.94E-06 -2.09E-06 5.80E-06 -4.83E-06 -2.05E-05 -2.37E-05
α5 5.07E-07 4.22E-07 -5.20E-08 -7.63E-08 -7.09E-07 -5.32E-07
α6 -3.96E-08 -1.19E-08 -2.87E-09 6.32E-08 1.44E-07 6.53E-08
α7 1.34E-09 2.56E-10 9.17E-10 -2.09E-09 -6.20E-09 -1.98E-09
α8 0 0 0 0 0 0
In the present embodiment, the optical physics parameter of the first lens to the 8th lens is as shown in the table:
Embodiment three:Fig. 3 is refer to, compared with embodiment one, the number amount and type of lens are essentially identical, but specifically Lens parameter and layout are different.
First lens 1 are convex-concave negative-power lenses, and second lens 2 are concavo-convex negative-power lenses, described 3rd lens 3 are biconvex positive power lens, and the 4th lens 4 are biconvex positive power lens, and the 5th lens 5 are double Recessed negative-power lenses, the 6th lens 6 are biconvex positive power lens, and the 7th lens 7 are that concave-concave negative power is saturating Mirror, the 8th lens 8 are convex-concave positive power lens.
First lens are as shown in the table to the 8th lens parameters:
F1=-11.5~-4.5 N1=1.43~1.85 R1=50~∞ R2=3.1~9
F2=-21.5~-12 N2=1.47~1.68 R3=-8.9~-3.1 R4=-40~-4.5
F3=6.5~15 N3=1.7~2.1 R5=5~50 R6=-40~-10
F4=6.5~15.5 N4=1.43~1.7 R7=5.5~19.7 R8=-9.2~-3
F5=-10~-3 N5=1.43~1.8 R9=-9.2~-3 R10=3.5~35
F6=6~12 N6=1.46~1.65 R11=5.6~19.2 R12=-18.5~-4.5
F7=-25~-7.5 N7=1.5~1.75 R13=-30~-5.6 R14=7~255
F8=10~30 N8=1.43~1.7 R15=5.3~16.5 R16=15~500
Meet that the asphericity coefficient of above-mentioned aspherical equation formula is as shown in the table in embodiment three:
In the present embodiment, the optical physics parameter of the first lens to the 8th lens is as shown in the table:
Face sequence number Face type R D nd K values
S1 Sphere 322 0.58 1.69
S2 Sphere 6.76 3
S3 It is aspherical -5.28 1.65 1.66 -0.47
S4 It is aspherical -10.43 0.07 -10.02
S5 Sphere 23 2.65 1.9
S6 Sphere -14.65 0.01
Diaphragm Plane PL 0.08
S7 Sphere 8.87 5 1.43
S8 Sphere -7.03
S9 Sphere -7.03 0.6 1.65
S10 Sphere 7.03 3.23
S11 It is aspherical 6.74 2.67 1.55 1.58
S12 It is aspherical -11.5 0.6 1.13
S13 It is aspherical -7.52 0.65 1.65 -18.2
S14 It is aspherical 168.7 0.8 106.88
S15 Sphere 8.13 1.745 1.55
S16 Sphere 39.48
The lens of three above embodiment have identical fastening means as follows:First lens are directly tight with the second lens Lean on, the second lens and the 3rd lens spacer ring close-fitting, the 3rd lens and the 4th lens are by spacer ring close-fitting, the 4th lens and the 5th saturating Mirror forms balsaming lens by gluing, and the 5th lens and the 6th lens pass through spacer ring close-fitting, the 6th lens and the 7th lens It is directly abutted against, the 7th lens and the 8th lens are abutted by spacer ring.
Above disclosed is only presently preferred embodiments of the present invention, it is impossible to the rights protection model of the present invention is limited with this Enclose, therefore the equivalent variations made according to scope of the present invention patent, still belong to the scope that the present invention is covered.

Claims (6)

1. a kind of large aperture 4K tight shots, including be arranged in order along optical axis from object space to image space the first lens, the second lens, 3rd lens, the 4th lens, the 5th lens, the 6th lens, the 7th lens and the 8th lens, it is characterised in that:Described first is saturating Mirror, the 3rd lens, the 4th lens, the 5th lens and the 8th lens are glass lens, second lens, the 6th lens and the 7th Lens are plastic aspheric lens.
A kind of 2. large aperture 4K tight shots according to claim 1, it is characterised in that:It is second lens, the 6th saturating Mirror and the 7th lens meet following conditional with whole camera lens respectively:
2<∣f2/f∣<6;
0.8<∣f6/f∣<4;
0.8<∣f7/f∣<5;
0.4<∣f6/f7∣<4.5;
Wherein, f is the focal length of whole camera lens, and f2, f6 and f7 correspond to Jiao of the second lens, the 6th lens and the 7th lens respectively Away from.
A kind of 3. large aperture 4K tight shots according to claim 2, it is characterised in that:4th lens and the 5th saturating Mirror is glued to form balsaming lens, and the balsaming lens meets following conditional with whole camera lens:
3.5<∣fe/f∣<80, wherein, fe is the focal length of balsaming lens.
A kind of 4. large aperture 4K tight shots according to any one of claims 1 to 3, it is characterised in that:Described first is saturating Mirror is convex-concave negative-power lenses, and second lens are concavo-convex negative-power lenses, and the 3rd lens are the positive light focuss of convex flat Lens are spent, the 4th lens are biconvex positive power lens, and the 5th lens are concave-concave negative-power lenses, the 6th lens It is biconvex positive power lens, the 7th lens are concave-concave negative-power lenses, and the 8th lens are biconvex positive power lens.
A kind of 5. large aperture 4K tight shots according to any one of claims 1 to 3, it is characterised in that:Described first is saturating Mirror is convex-concave negative-power lenses, and second lens are concavo-convex negative-power lenses, and the 3rd lens are the positive light focuss of biconvex Lens are spent, the 4th lens are biconvex positive power lens, and the 5th lens are concave-concave negative-power lenses, the described 6th Lens are biconvex positive power lens, and the 7th lens are concave-concave negative-power lenses, and the 8th lens are the positive light of biconvex Power lenses.
A kind of 6. large aperture 4K tight shots according to any one of claims 1 to 3, it is characterised in that:Described first is saturating Mirror is convex-concave negative-power lenses, and second lens are concavo-convex negative-power lenses, and the 3rd lens are the positive light focuss of biconvex Lens are spent, the 4th lens are biconvex positive power lens, and the 5th lens are concave-concave negative-power lenses, the described 6th Lens are biconvex positive power lens, and the 7th lens are concave-concave negative-power lenses, and the 8th lens are the positive light of convex-concave Power lenses.
CN201710833067.7A 2017-09-15 2017-09-15 A kind of large aperture 4K tight shots Pending CN107367828A (en)

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Cited By (6)

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CN108845405A (en) * 2018-09-25 2018-11-20 云南博硕信息技术有限公司 Wide spectrum double-view field monitoring camera dual-purpose round the clock
CN109507785A (en) * 2018-12-26 2019-03-22 东莞市宇瞳光学科技股份有限公司 A kind of infrared confocal camera lens
CN109541780A (en) * 2018-11-16 2019-03-29 江西联创电子有限公司 Optical lens and imaging device
CN110488470A (en) * 2018-05-14 2019-11-22 宁波舜宇车载光学技术有限公司 Optical lens
WO2020143420A1 (en) * 2019-01-07 2020-07-16 广东弘景光电科技股份有限公司 High-resolution, wide angle, day and night confocal optical system and camera module used by same
WO2021168662A1 (en) * 2020-02-25 2021-09-02 天津欧菲光电有限公司 Optical system, lens module, and terminal device

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Inventor after: Zhang Pinguang

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Application publication date: 20171121