CN203759346U - Novel long-wave infrared prime lens - Google Patents
Novel long-wave infrared prime lens Download PDFInfo
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- CN203759346U CN203759346U CN201420159672.2U CN201420159672U CN203759346U CN 203759346 U CN203759346 U CN 203759346U CN 201420159672 U CN201420159672 U CN 201420159672U CN 203759346 U CN203759346 U CN 203759346U
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- 230000003287 optical effect Effects 0.000 claims abstract description 59
- 239000000463 material Substances 0.000 claims abstract description 25
- 239000005387 chalcogenide glass Substances 0.000 claims abstract description 13
- 230000005499 meniscus Effects 0.000 claims abstract description 6
- 239000000203 mixture Substances 0.000 claims description 3
- 238000012544 monitoring process Methods 0.000 abstract 1
- 238000005516 engineering process Methods 0.000 description 4
- 238000003384 imaging method Methods 0.000 description 4
- 201000009310 astigmatism Diseases 0.000 description 2
- 230000000694 effects Effects 0.000 description 2
- 230000001154 acute effect Effects 0.000 description 1
- 230000004075 alteration Effects 0.000 description 1
- 238000010923 batch production Methods 0.000 description 1
- 230000009286 beneficial effect Effects 0.000 description 1
- 230000015556 catabolic process Effects 0.000 description 1
- 238000010276 construction Methods 0.000 description 1
- 238000006731 degradation reaction Methods 0.000 description 1
- 238000007723 die pressing method Methods 0.000 description 1
- 238000009826 distribution Methods 0.000 description 1
- 238000004519 manufacturing process Methods 0.000 description 1
- 230000035800 maturation Effects 0.000 description 1
- 238000000034 method Methods 0.000 description 1
- 230000004297 night vision Effects 0.000 description 1
- 238000005498 polishing Methods 0.000 description 1
- 238000003825 pressing Methods 0.000 description 1
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Abstract
The utility model provides a novel long-wave infrared prime lens. The novel long-wave infrared prime lens is characterized in that three lenses are sequentially arranged along the optical axis from an object space to an image space, the first lens is a meniscus lens with positive refractive power, a convex surface of the meniscus lens faces the object space, the second lens is a lens with negative refractive power, the third lens is a lens with positive refractive power, a convex surface of the third lens faces the image space, the novel long-wave infrared prime lens meets formulas that FNOXf12Xf3X(n1-1)/(fXfXR1) is larger than 0 and smaller than 1 and dn1/dT is larger than 1X10<-5> and smaller than 5X10<-5>, the f is the focal length of an integral optical system, the n1 is a central wavelength refractive index of materials of the first lens, the FNO is an F number of the optical system, the f12 is a combined focal length of the first lens and the second lens, the f3 is the focal length of the third lens, the R1 is an approximate curvature radius of the first lens, and the dn1/dT is a temperature coefficient of the refractive index of the materials of the first lens. The novel long-wave infrared prime lens has the advantages that the novel long-wave infrared prime lens is made of three types of chalcogenide glass materials, is simple in structure and reliable in performance and can be applied to infrared vehicular assisting and security and protection monitoring fields with the requirement on realizing a heat difference eliminating function in wide temperature ranges.
Description
Technical field
The utility model relates to a kind of novel LONG WAVE INFRARED tight shot, especially one and has the poor performance of the heat that disappears in wide temperature range, can be widely used in the LONG WAVE INFRARED tight shot of on-vehicle night vision and protection and monitor field.
Background technology
Along with the maturation of uncooled detector technology, LWIR Uncooled Optical System is all widely used in dual-use field.Because the thermal refractive index coefficient of infrared optical material is larger, the acute variation of working temperature can have serious impact to infrared optical system, causes degradation problem under system focal length variations, image planes drift, image quality.Must disappearing for the infrared optical system of these special application fields, heat is poor to be designed, and in design, considers the impact of temperature variation on system imaging quality, makes infrared optical system all have good image quality in a larger temperature range.
Disappearing in heat difference technology of infrared optical system, optics disappears heat difference because the features such as it is simple in structure, dependable performance are widely used.But existing optics disappears there is following problem in the poor camera lens scheme of heat, the one, and utilize multiple material thermal characteristics difference to coordinate realization to disappear hot poor, this scheme exists and uses material many, and number of shots is more, structure relative complex, high in cost of production problem; The 2nd, adopt utilize diffraction optical element to there is the loose characteristic of the negative heat that disappears to realize the heat that disappears poor, this scheme existence is because the diffraction efficiency of diffraction surfaces causes the transmissivity of optical system obvious problem that declines.
Utility model content
The utility model is in order to have solved the above-mentioned optics problem existing in poor system that disappears, a kind of novel LONG WAVE INFRARED optics tight shot is provided, this system adopts three-chip type structure, utilize chalcogenide glass to there is the characteristic of lower thermal refractive index coefficient, realize the poor characteristic of the heat that disappears in wide temperature range.
The technical scheme that the utility model solves the problems of the technologies described above is as described below:
A kind of novel LONG WAVE INFRARED optics tight shot, is disposed with first lens L1, the second lens L2 and the 3rd lens L3 along optical axis from object space to image space;
Described first lens is to have positive refractive power the convex surface meniscus lens to thing side;
The second described lens are the lens with negative refractive power;
The 3rd described lens are to have positive refractive power the convex surface lens to picture side;
Described novel LONG WAVE INFRARED tight shot meets following formula:
0<FNO*f12*f3* (n1-1)/(f*f*R1) <1 and 1*10
-5<dn1/dT<5*10
-5
Wherein, the focal length that f is whole optical system; N1 is the centre wavelength refractive index of first lens material; FNO is the F number of optical system; F12 is the combined focal length of first lens and the second lens; F3 is the focal length of the 3rd lens; The approximate radius-of-curvature of convex surface of R1 first lens; Dn1/dT is first lens Refractive Index of Material temperature coefficient.
Described the 3rd lens meet following expression formula further:
1*10
-5<dn3/dT<5*10
-5
Wherein, n3 is the centre wavelength refractive index of first lens material; Dn3/dT is first lens Refractive Index of Material temperature coefficient.
Further, combined focal length and the optical system focal length of described first lens and the second lens composition meet following expression formula:
1<f12/f<7
Wherein, f12 is the combined focal length of first lens and the second lens; F is the focal length of whole optical system.
Further, described first lens and optical system focal length meet following expression formula:
0<f1/f<1
Wherein, f1 is first lens focal length; F is the focal length of whole optical system.
Further, described the second lens and optical system focal length meet following expression formula:
-1<f2/f<0
Wherein, f2 is second focal length of lens; F is the focal length of whole optical system.
Further, described the 3rd lens and optical system focal length meet following expression formula:
0<f3/f<1
Wherein, f3 is the 3rd focal length of lens; F is the focal length of whole optical system.
Further, described camera lens adopts three kinds of chalcogenide glass materials, and each lens adopts different chalcogenide glass materials.
In the lens of described camera lens, all do not contain diffraction surfaces structure.
The utility model compared with prior art, has following advantage and beneficial effect:
The utility model, by adopting the scheme of three lens, is realized the poor function of the heat that disappears in wide temperature range without adopting diffraction surfaces structure.The more existing optics poor scheme of heat that disappears has following advantage: realize optics with multiple optical material proportioning and disappear compared with the poor scheme of heat, the utlity model has lens wearer quantity few, the simple advantage of lens construction; With adopt diffraction optical element to realize optics to disappear compared with the poor scheme of heat, the utility model, due to without adopting diffraction surfaces structure, has advantages of that system transmitance is high.The utility model adopt three kinds of chalcogenide glasses, in material cost, chalcogenide glass has obvious advantage, and chalcogenide glass produce in enormous quantities time can carry out accurate die pressing, can greatly cut down finished cost, there are wide market outlook.Facts have proved, this kind of technical scheme has good effect.
Brief description of the drawings
By the description of its exemplary embodiment being carried out below in conjunction with accompanying drawing, the above-mentioned feature and advantage of the utility model will become apparent and easily understand.
Fig. 1 is the structural representation of the specific embodiment of novel LONG WAVE INFRARED tight shot described in the utility model;
Fig. 2 is the chromatic curve figure (mm) of specific embodiment;
Fig. 3 is the astigmatism curve map (mm) of specific embodiment;
Fig. 4 is the distortion curve figure (%) of specific embodiment;
Fig. 5 is the MTF curve map of specific embodiment.
Embodiment
Fig. 1 is the structural representation of LONG WAVE INFRARED tight shot described in the utility model.
As shown in Figure 1, described LONG WAVE INFRARED tight shot, it is disposed with from the object side to image side along optical axis: have the first lens L1 of positive refractive power, system stop St is positioned on first surface; There is the second lens L2 of negative refractive power; There is the 3rd lens L3 and the imaging surface 100 of positive refractive power.Incident light, by first lens L1, enters the second lens L2 and the 3rd lens L3, finally assembles and enters among imaging surface 100.
Wherein, in this infrared optical system, first lens L1 is the positive meniscus lens of convex surface towards thing side; The second lens L2 is the diverging meniscus lens of convex surface towards thing side; The 3rd lens L3 is the lens of convex surface towards picture side.The concave surface R2 of first lens L1 is aspheric surface, and the concave surface R4 of the second lens L2 is aspheric surface, and all the other are sphere.
From thing side to picture side, the two sides of described first lens L1 is R1, R2, and the two sides of described the second lens L2 is R3, R4, and the two sides of described the 3rd lens L3 is R5, R6, described Z1 refers to the central optical axis of camera lens, along on central optical axis, the thickness of described first lens L1 is D1, with the distance of the second lens L2 be D2, the thickness of described the second lens L2 is D3, with the distance of the 3rd lens L3 be D4, the thickness of described the 3rd lens L3 is D5, with the distance of imaging surface 100 be D6.
Described first lens L1, the second lens L2, the material of the 3rd lens L3 is chalcogenide glass, has good transmitance at 8～12 μ m, and transparent region covers three atmospheric windows.It is less that chalcogenide glass refractive index varies with temperature coefficient d n/dT, adopts chalcogenide glass to add that rational focal power distribution can realize the good poor function of the heat that disappears in optical system.On processing mode, chalcogenide glass can polishing except having, can turning, and maximum characteristic can also high-accuracy mold pressing, has great cost advantage in the time of batch production.
This optical system is in the time of design, and for reaching the high score rate picture element requirement of 384*28825 micron detector, camera lens diaphragm is placed on the first surface of first lens L1.Described novel LONG WAVE INFRARED tight shot meets following formula:
0<FNO*f12*f3* (n1-1)/(f*f*R1) <1 and 1*10
-5<dn1/dT<5*10
-5
Wherein, the focal length that f is whole optical system; N1 is the centre wavelength refractive index of first lens material; FNO is the F number of optical system; F12 is the combined focal length of first lens and the second lens; F3 is the focal length of the 3rd lens; The approximate radius-of-curvature of convex surface of R1 first lens; Dn1/dT is first lens Refractive Index of Material temperature coefficient.
Further, described the 3rd lens meet following expression formula:
1*10
-5<dn3/dT<5*10
-5
Wherein, n3 is the centre wavelength refractive index of first lens material; Dn3/dT is first lens Refractive Index of Material temperature coefficient.
Further, combined focal length and the optical system focal length of described first lens and the second lens composition meet following expression formula:
1<f12/f<7
Wherein, f12 is the combined focal length of first lens and the second lens; F is the focal length of whole optical system.
Further, described first lens and optical system focal length meet following expression formula:
0<f1/f<1
Wherein, f1 is first lens focal length; F is the focal length of whole optical system.
Further, described the second lens and optical system focal length meet following expression formula:
-1<f2/f<0
Wherein, f2 is second focal length of lens; F is the focal length of whole optical system.
Further, described the 3rd lens and optical system focal length meet following expression formula:
0<f3/f<1
Wherein, f3 is the 3rd focal length of lens; F is the focal length of whole optical system.
In the present embodiment, the focal distance f=22mm of this optical system, f-number FNO=1.1.The approximate radius of curvature R 1=17.04 of convex surface of first lens L1, the focal distance f 1=13.35mm of first lens L1, the focal length of the second lens L2 is f2=-10.14mm, the focal length of the 3rd lens L3 is f3=16.01mm, the combined focal length f12=102.143mm of first lens and the second lens, the refractive index n 1=2.7776 of first lens;
FNO*f12*f3*(n1-1)/(f*f*R1)=0.39；
f12/f=4.64；
f1/f=0.61；
f2/f=-0.46；
f3/f=0.73；
dn1/dT=4.1*10
-5；
dn3/dT=3.6*10
-5；
Fig. 2 to Fig. 5 is the optical indicatrix figure of corresponding embodiment, and wherein Fig. 2 is that chromatic curve figure is represented by three wavelength of 8 μ m, 10 μ m, 12 μ m, and unit is mm.Fig. 3 is astigmatism curve map, is represented equally by three wavelength of 8 μ m, 10 μ m, 12 μ m, and unit is mm.Fig. 4 is distortion curve figure, indicates the distortion sizes values under different field angle, and unit is %.Fig. 5 is MTF curve map, represents that the comprehensive solution of optical system is as level, and up-to-date 384*28825 μ m request detector reaches 20 lines to resolution.As seen from the figure, this LONG WAVE INFRARED optical system, by various optical aberration correctings, is enough to meet real requirement.
The utility model optical system parameter refers to table one, table two.
Table one, optical component parameter table
Described aspheric surface meets following expression formula:
In formula, Z is aspheric surface along optical axis direction when highly for the position of Y, and apart from the distance rise Sag on aspheric surface summit, R represents the paraxial radius-of-curvature of minute surface, and k is circular cone coefficient conic, and A, B, C, D are high order aspheric surface coefficient.
Table two: aspherical surface data
| Aspheric surface | K | A | B | C | D |
| 2 | 0 | 8.281593E-006 | 2.489640E-008 | -4.055192E-011 | -2.500404E-013 |
| 4 | 0 | 2.106796E-005 | -1.016960E-007 | -2.175333E-009 | -2.505533E-012 |
It should be noted that the design parameter in above table is only exemplary, the parameter of each lens is not limited to, by the shown value of above-mentioned each numerical example, can adopt other value, can reach similar technique effect.
Although described principle of the present utility model and embodiment above; but; under above-mentioned instruction of the present utility model; those skilled in the art can carry out various improvement and distortion on the basis of above-described embodiment, and these improvement or distortion drop in protection domain of the present utility model.It will be understood by those skilled in the art that specific descriptions are above in order to explain the purpose of this utility model, not for limiting the utility model.Protection domain of the present utility model is limited by claim and equivalent thereof.
Claims (8)
1. a novel LONG WAVE INFRARED tight shot, it is characterized in that: be disposed with first lens, the second lens, the 3rd lens along optical axis from object space to image space, wherein, described first lens is the meniscus shaped lens with positive refractive power of convex surface towards thing side, the second lens are the lens with negative refractive power, and the 3rd lens are that convex surface is towards the lens with positive refractive power as side; Described novel LONG WAVE INFRARED tight shot meets following formula:
0<FNO*f12*f3* (n1-1)/(f*f*R1) <1 and 1*10
-5<dn1/dT<5*10
-5
Wherein, the focal length that f is whole optical system; N1 is the centre wavelength refractive index of first lens material; FNO is the F number of optical system; F12 is the combined focal length of first lens and the second lens; F3 is the focal length of the 3rd lens; R1 is the approximate radius-of-curvature of the convex surface of first lens; Dn1/dT is the Refractive Index of Material temperature coefficient of first lens.
2. novel LONG WAVE INFRARED tight shot according to claim 1, is characterized in that: described the 3rd lens meet following expression formula:
1*10
-5<dn3/dT<5*10
-5
Wherein, n3 is the centre wavelength refractive index of first lens material; Dn3/dT is first lens Refractive Index of Material temperature coefficient.
3. novel LONG WAVE INFRARED tight shot according to claim 1, is characterized in that: combined focal length and the optical system focal length of described first lens and the second lens composition meet following expression formula:
1<f12/f<7
Wherein, f12 is the combined focal length of first lens and the second lens; F is the focal length of whole optical system.
4. novel LONG WAVE INFRARED tight shot according to claim 1, is characterized in that: the focal length of described first lens and optical system focal length meet following expression formula:
0<f1/f<1
Wherein, the focal length that f1 is first lens; F is the focal length of whole optical system.
5. novel LONG WAVE INFRARED tight shot according to claim 1, is characterized in that: the focal length of described the second lens and optical system focal length meet following expression formula:
-1<f2/f<0
Wherein, f2 is the focal length of the second lens; F is the focal length of whole optical system.
6. novel LONG WAVE INFRARED tight shot according to claim 1, is characterized in that: the focal length of described the 3rd lens and optical system focal length meet following expression formula:
0<f3/f<1
Wherein, f3 is the focal length of the 3rd lens; F is the focal length of whole optical system.
7. novel LONG WAVE INFRARED tight shot according to claim 1, is characterized in that: described camera lens adopts three kinds of chalcogenide glass materials, and each lens adopts different chalcogenide glass materials.
8. novel LONG WAVE INFRARED tight shot according to claim 1, is characterized in that: in the lens of described camera lens, all do not contain diffraction surfaces structure.
Priority Applications (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| CN201420159672.2U CN203759346U (en) | 2014-04-02 | 2014-04-02 | Novel long-wave infrared prime lens |
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| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| CN201420159672.2U CN203759346U (en) | 2014-04-02 | 2014-04-02 | Novel long-wave infrared prime lens |
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| CN203759346U true CN203759346U (en) | 2014-08-06 |
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Cited By (2)
| Publication number | Priority date | Publication date | Assignee | Title |
|---|---|---|---|---|
| CN103941379A (en) * | 2014-04-02 | 2014-07-23 | 宁波舜宇红外技术有限公司 | Novel long wave infrared prime camera lens |
| CN113589475A (en) * | 2021-07-02 | 2021-11-02 | 支付宝(杭州)信息技术有限公司 | Projection lens suitable for 3D face recognition |
-
2014
- 2014-04-02 CN CN201420159672.2U patent/CN203759346U/en not_active Expired - Lifetime
Cited By (3)
| Publication number | Priority date | Publication date | Assignee | Title |
|---|---|---|---|---|
| CN103941379A (en) * | 2014-04-02 | 2014-07-23 | 宁波舜宇红外技术有限公司 | Novel long wave infrared prime camera lens |
| CN103941379B (en) * | 2014-04-02 | 2016-06-15 | 宁波舜宇红外技术有限公司 | A kind of novel LONG WAVE INFRARED tight shot |
| CN113589475A (en) * | 2021-07-02 | 2021-11-02 | 支付宝(杭州)信息技术有限公司 | Projection lens suitable for 3D face recognition |
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| C14 | Grant of patent or utility model | ||
| GR01 | Patent grant | ||
| CX01 | Expiry of patent term | ||
| CX01 | Expiry of patent term |
Granted publication date: 20140806 |