CN111638586A - Glass-plastic mixed infrared confocal lens - Google Patents
Glass-plastic mixed infrared confocal lens Download PDFInfo
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- CN111638586A CN111638586A CN202010660266.4A CN202010660266A CN111638586A CN 111638586 A CN111638586 A CN 111638586A CN 202010660266 A CN202010660266 A CN 202010660266A CN 111638586 A CN111638586 A CN 111638586A
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- G—PHYSICS
- G02—OPTICS
- G02B—OPTICAL ELEMENTS, SYSTEMS OR APPARATUS
- G02B13/00—Optical objectives specially designed for the purposes specified below
- G02B13/001—Miniaturised objectives for electronic devices, e.g. portable telephones, webcams, PDAs, small digital cameras
- G02B13/0015—Miniaturised objectives for electronic devices, e.g. portable telephones, webcams, PDAs, small digital cameras characterised by the lens design
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- G—PHYSICS
- G02—OPTICS
- G02B—OPTICAL ELEMENTS, SYSTEMS OR APPARATUS
- G02B13/00—Optical objectives specially designed for the purposes specified below
- G02B13/001—Miniaturised objectives for electronic devices, e.g. portable telephones, webcams, PDAs, small digital cameras
- G02B13/0015—Miniaturised objectives for electronic devices, e.g. portable telephones, webcams, PDAs, small digital cameras characterised by the lens design
- G02B13/002—Miniaturised objectives for electronic devices, e.g. portable telephones, webcams, PDAs, small digital cameras characterised by the lens design having at least one aspherical surface
- G02B13/0045—Miniaturised 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
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- G—PHYSICS
- G02—OPTICS
- G02B—OPTICAL ELEMENTS, SYSTEMS OR APPARATUS
- G02B13/00—Optical objectives specially designed for the purposes specified below
- G02B13/001—Miniaturised objectives for electronic devices, e.g. portable telephones, webcams, PDAs, small digital cameras
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Abstract
The invention relates to the technical field of lenses. The invention discloses a glass-plastic mixed infrared confocal lens which sequentially comprises a first lens, a second lens, a third lens and a fourth lens from an object side to an image side along an optical axis; the first lens is a convex-concave lens with negative refractive index; the second lens has positive refractive index; the third lens and the fifth lens are both convex lenses with positive refraction; the fourth lens element has negative refractive index; the first lens and the third lens are both glass spherical lenses, and the second lens, the fourth lens and the fifth lens are all plastic aspheric lenses; the temperature coefficient of the refractive index of the third lens is a negative value. The invention has the advantages of small temperature drift; the pixels are high, and the imaging quality is good; the light transmission is large, and the contrast is high; the day and night confocality is good; low cost.
Description
Technical Field
The invention belongs to the technical field of lenses, and particularly relates to a glass-plastic mixed infrared confocal lens.
Background
With the continuous progress of scientific technology and the continuous development of society, in recent years, optical imaging lenses are also rapidly developed, and the optical imaging lenses are widely applied to various fields such as smart phones, tablet computers, video conferences, vehicle-mounted monitoring, security monitoring, unmanned aerial vehicles aerial photography, machine vision systems and the like, so that the requirements on the optical imaging lenses are higher and higher.
However, the existing optical imaging lens for security monitoring has many defects, such as the adoption of all-glass lens design, which results in high cost; the imaging stability is easily influenced by external temperature, and the temperature drift control is poor; the pixel is usually only about three million, the image quality is not high, and the infrared imaging quality is difficult to ensure; the clear aperture is generally small, the imaging edge contrast value is low, and the like, and therefore, improvements are necessary to meet the increasing demands of consumers.
Disclosure of Invention
The invention aims to provide a glass-plastic mixed infrared confocal lens to solve the technical problems.
In order to achieve the purpose, the invention adopts the technical scheme that: a glass-plastic mixed infrared confocal lens comprises a first lens, a second lens, a third lens, a fourth lens, a fifth lens and a fourth lens, wherein the first lens, the second lens and the fifth lens are sequentially arranged from an object side to an image side along an optical axis; the first lens, the second lens, the third lens and the fourth lens are respectively arranged on the object side and the image side, and the object side faces towards the object side and enables the imaging light rays to pass through;
the first lens element with negative refractive index has a convex object-side surface and a concave image-side surface;
the second lens has positive refractive index;
the third lens element with positive refractive index has a convex object-side surface and a convex image-side surface;
the fourth lens element has negative refractive index;
the fifth lens element with positive refractive index has a convex object-side surface and a convex image-side surface;
the first lens and the third lens are both glass spherical lenses, and the second lens, the fourth lens and the fifth lens are all plastic aspheric lenses;
the temperature coefficient of the refractive index of the third lens is a negative value;
the glass-plastic mixed infrared confocal lens is provided with the lenses with the refractive index only from the first lens to the fifth lens.
Further, this glass is moulded and is mixed infrared confocal camera lens and still satisfy: nd1>1.75, where nd1 is the refractive index of the first lens.
Further, this glass is moulded and is mixed infrared confocal camera lens and still satisfy: nd2>1.6, nd4>1.6, where nd2 is the refractive index of the second lens and nd4 is the refractive index of the fourth lens.
Further, the second lens, the fourth lens and the fifth lens are all high-order even-order aspheric lenses.
Furthermore, the first lens and the second lens are connected by a lens cone bearing platform.
Furthermore, the edge of the fourth lens is directly abutted and jointed with the edge of the fifth lens.
Further, this glass is moulded and is mixed infrared confocal camera lens and still satisfy: 6.5< f2/f <9, 1.5< f3/f <3 and 1< f5/f <2, wherein f is the focal length of the glass-plastic hybrid infrared confocal lens, f2 is the focal length of the second lens, f3 is the focal length of the third lens, and f5 is the focal length of the fifth lens.
Further, this glass is moulded and is mixed infrared confocal camera lens and still satisfy: -7mm < f1< -4mm, 21mm < f2<23mm, 6mm < f3<8mm, -5mm < f4< -3mm and 3mm < f5<5mm, wherein f1, f2, f3, f4, f5 are the focal lengths of the first lens, the second lens, the third lens, the fourth lens and the fifth lens, respectively.
Further, this glass is moulded and is mixed infrared confocal camera lens and still satisfy: 14mm < R11<16mm, 2mm < R12<4mm, -6mm < R21< -4mm, -6mm < R22< -4mm, 13mm < R31<16mm, -7mm < R32< -5mm, 10mm < R41<13mm, 2mm < R42<4mm, 3mm < R51<5mm, and-6 mm < R52< -4mm, wherein R11, R21, R31, R41, and R51 are radii of curvature of object sides of the first lens, the second lens, the third lens, the fourth lens, and the fifth lens, and R12, R22, R32, R42, and R52 are radii of curvature of image sides of the first lens, the second lens, the third lens, the fourth lens, and the fifth lens, respectively.
Further, this glass is moulded and is mixed infrared confocal camera lens and still satisfy: 0.3< D11/R11<0.7 and 0.3< D31/R31<0.7, wherein D11 and D31 are clear apertures of object-side surfaces of the first lens and the third lens, respectively, and R11 and R31 are radii of curvature of the object-side surfaces of the first lens and the third lens, respectively.
The invention has the beneficial technical effects that:
the invention adopts five lenses and glass-plastic mixed design, and has low cost and industrial mass production feasibility by correspondingly designing each lens; the temperature drift control is good, and when the temperature drift control is used in a range of-40 ℃ to 85 ℃, an image picture is not distorted; the image surface is large, the pixels are high and can reach five million pixels, and the imaging quality is good; the light passes through greatly, and when switching infrared imaging, infrared offset is little, the advantage that day and night confocality is good.
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 introduced below, and it is obvious that the drawings in the following description are only some embodiments of the present invention, and it is obvious for those skilled in the art to obtain other drawings based on these drawings without creative efforts.
FIG. 1 is a schematic structural diagram according to a first embodiment of the present invention;
FIG. 2 is a graph of MTF of 425-675nm visible light according to the first embodiment of the present invention;
FIG. 3 is a defocus plot of visible light at 425 and 675nm at 60lp/mm in the first embodiment of the present invention;
FIG. 4 is a schematic diagram of a lateral chromatic aberration curve according to a first embodiment of the present invention;
FIG. 5 is a graph of relative illumination at 550nm according to a first embodiment of the present invention;
FIG. 6 is a dot-column diagram according to a first embodiment of the present invention;
FIG. 7 is an MTF graph of infrared 820-880nm according to the first embodiment of the present invention;
FIG. 8 is a defocus plot at 60lp/mm for infrared 820-880nm in accordance with the first embodiment of the present invention;
FIG. 9 is a schematic structural diagram according to a second embodiment of the present invention;
FIG. 10 is a graph of the MTF at 675nm of visible light 425 and the second embodiment of the present invention;
FIG. 11 is a defocus plot of 425-675nm visible light at 60lp/mm in the second embodiment of the present invention;
FIG. 12 is a schematic diagram of a lateral chromatic aberration curve according to a second embodiment of the present invention;
FIG. 13 is a graph of contrast at 550nm for example two of the present invention;
FIG. 14 is a dot diagram according to a second embodiment of the present invention;
FIG. 15 is an MTF graph at 820-880nm according to the second embodiment of the present invention;
FIG. 16 is a defocus plot at 60lp/mm for infrared 820-880nm in accordance with the second embodiment of the present invention;
FIG. 17 is a schematic structural diagram of a third embodiment of the present invention;
FIG. 18 is the MTF graph of 425-675nm visible light in the third embodiment of the present invention;
FIG. 19 is a defocus plot of 425 and 675nm visible light at 60lp/mm in a third embodiment of the present invention;
FIG. 20 is a schematic diagram of a lateral chromatic aberration curve according to a third embodiment of the present invention;
FIG. 21 is a graph of contrast at 550nm for example three of the present invention;
FIG. 22 is a dot diagram of a third embodiment of the present invention;
FIG. 23 is an MTF graph of infrared 820-880nm according to the third embodiment of the present invention;
FIG. 24 is a defocus plot at 60lp/mm for infrared 820-880nm in the third embodiment of the present invention;
FIG. 25 is a schematic structural diagram according to a fourth embodiment of the present invention;
FIG. 26 is the MTF graph of 425-675nm visible light according to the fourth embodiment of the present invention;
FIG. 27 is a defocus plot of 425 and 675nm visible light at 60lp/mm in the fourth embodiment of the present invention;
FIG. 28 is a schematic diagram of a lateral chromatic aberration curve according to a fourth embodiment of the present invention;
FIG. 29 is a graph of contrast at 550nm for example four of the present invention;
FIG. 30 is a dot diagram according to a fourth embodiment of the present invention;
FIG. 31 is an MTF plot at 820 and 880nm in accordance with the fourth embodiment of the present invention;
FIG. 32 is a defocus plot at 60lp/mm for infrared 820-880nm in accordance with the fourth embodiment of the present invention;
FIG. 33 is a schematic structural diagram of a fifth embodiment of the present invention;
FIG. 34 is the MTF graph of visible light 425 and 675nm of the fifth embodiment of the present invention;
FIG. 35 is the defocus plot of visible light 425 and 675nm at 60lp/mm in the fifth embodiment of the present invention;
FIG. 36 is a schematic diagram of a lateral chromatic aberration curve according to a fifth embodiment of the present invention;
FIG. 37 is a contrast plot at 550nm for example five of the present invention;
FIG. 38 is a dot diagram of a fifth embodiment of the present invention;
FIG. 39 is the MTF graph at 820 and 880nm in the fifth embodiment of the present invention;
FIG. 40 is a defocus graph of 60lp/mm at infrared 820-880nm in accordance with the fifth embodiment of the present invention.
Detailed Description
To further illustrate the various embodiments, the 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. Those skilled in the art will appreciate still other possible embodiments and advantages of the present invention with reference to these figures. Elements in the figures are not drawn to scale and like reference numerals are generally used to indicate like elements.
The invention will now be further described with reference to the accompanying drawings and detailed description.
The term "a lens element having positive refractive index (or 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 passing 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 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 invention discloses a glass-plastic mixed infrared confocal lens which sequentially comprises a first lens, a second lens, a third lens and a fourth lens from an object side to an image side along an optical axis; the first lens element to the fifth lens element each include an object-side surface facing the object side and passing the image light and an image-side surface facing the image side and passing the image light.
The first lens element with negative refractive index has a convex object-side surface and a concave image-side surface.
The second lens element has a positive refractive index.
The third lens element with positive refractive power has a convex object-side surface and a convex image-side surface.
The fourth lens element has a negative refractive index.
The fifth lens element with positive refractive power has a convex object-side surface and a convex image-side surface.
First lens and third lens are glass spherical lens, and second lens, fourth lens and fifth lens are plastics aspheric lens, and second lens, fourth lens and fifth lens adopt the aspheric surface, can correct the high order aberration well, promote image reducibility, reduce image noise value, and plastics aspheric lens simultaneously all shares manufacturing cost for low cost easily extensive volume production is used, and the practicality is high.
The temperature coefficient of the refractive index of the third lens is a negative value, so that the influence of external temperature change on the back focus of the lens can be well counteracted, and the clear and non-defocusing picture can be ensured when the lens is used in a temperature range of-40 ℃ to 85 ℃.
The glass-plastic mixed infrared confocal lens is provided with the lenses with the refractive index only from the first lens to the fifth lens. The invention adopts five lenses and glass-plastic mixed design, and has low cost and industrial mass production feasibility by correspondingly designing each lens; the temperature drift control is good, and when the temperature drift control is used in a range of-40 ℃ to 85 ℃, an image picture is not distorted; the image surface is large, the pixels are high and can reach five million pixels, and the imaging quality is good; the light passes through greatly, and when switching infrared imaging, infrared offset is little, the advantage that day and night confocality is good.
Preferably, this glass is moulded and is mixed infrared confocal camera lens and still satisfy: nd1>1.75, where nd1 is the refractive index of the first lens, which is advantageous for integrating the field of view, making the lens outer diameter not too large.
Preferably, this glass is moulded and is mixed infrared confocal camera lens and still satisfy: nd2>1.6, nd4>1.6, wherein nd2 is the refractive index of the second lens, and nd4 is the refractive index of the fourth lens, further improving the light transmission amount and the pixels.
Preferably, the second lens, the fourth lens and the fifth lens are all high-order even-order aspheric lenses, so that aberration is further eliminated, and imaging quality is improved.
Preferably, the first lens and the second lens are connected by a lens cone bearing platform, so that the assembly precision can be effectively improved.
Preferably, the edges of the fourth lens and the fifth lens are directly abutted and connected without using a spacer ring, so that the influence on two aspheric surfaces caused by extrusion of the spacer ring in the assembling process is avoided, and the assembling yield of finished products is improved.
Preferably, this glass is moulded and is mixed infrared confocal camera lens and still satisfy: 6.5< f2/f <9, 1.5< f3/f <3, and 1< f5/f <2, where f is the focal length of the glass-plastic hybrid infrared confocal lens, f2 is the focal length of the second lens, f3 is the focal length of the third lens, and f5 is the focal length of the fifth lens, further managing and controlling the temperature drift of the system.
Preferably, this glass is moulded and is mixed infrared confocal camera lens and still satisfy: 7mm < f1< -4mm, 21mm < f2<23mm, 6mm < f3<8mm, -5mm < f4< -3mm and 3mm < f5<5mm, wherein f1, f2, f3, f4 and f5 are focal lengths of the first lens, the second lens, the third lens, the fourth lens and the fifth lens respectively, and further control the temperature drift of the system.
Preferably, this glass is moulded and is mixed infrared confocal camera lens and still satisfy: 14mm < R11<16mm, 2mm < R12<4mm, -6mm < R21< -4mm, -6mm < R22< -4mm, 13mm < R31<16mm, -7mm < R32< -5mm, 10mm < R41<13mm, 2mm < R42<4mm, 3mm < R51<5mm, and-6 mm < R52< -4mm, wherein R11, R21, R31, R41, and R51 are curvature radii of object side surfaces of the first lens, the second lens, the third lens, the fourth lens, and the fifth lens, and R12, R22, R32, R42, and R52 are curvature radii of side surfaces of the first lens, the second lens, the third lens, the fourth lens, and the fifth lens, respectively, and are easy to machine and reduce detection difficulty.
Preferably, this glass is moulded and is mixed infrared confocal camera lens and still satisfy: 0.3< D11/R11<0.7 and 0.3< D31/R31<0.7, wherein D11 and D31 are the clear aperture of the object side surfaces of the first lens and the third lens, respectively, and R11 and R31 are the curvature radii of the object side surfaces of the first lens and the third lens, respectively, which is favorable for correcting edge distortion.
The glass-plastic hybrid infrared confocal lens of the present invention will be described in detail with specific examples.
Example one
As shown in fig. 1, a glass-plastic hybrid infrared confocal lens includes, in order from an object side a1 to an image side a2 along an optical axis I, a first lens 1, a second lens 2, a stop 6, a third lens 3, a fourth lens 4, a fifth lens 5, a protective glass 7, and an image plane 8; the first lens element 1 to the fifth lens element 5 each include an object-side surface facing the object side a1 and passing the imaging light rays, and an image-side surface facing the image side a2 and passing the imaging light rays.
The first lens element 1 has a negative refractive index, and an object-side surface 11 of the first lens element 1 is convex and an image-side surface 12 of the first lens element 1 is concave.
The second lens element 2 has a positive refractive index, the object-side surface 21 of the second lens element 2 is concave, and the image-side surface 22 of the second lens element 2 is convex, but the disclosure is not limited thereto, and in some embodiments, the object-side surface of the second lens element may be convex and the image-side surface of the second lens element may be concave.
The object-side surface 21 and the image-side surface 22 of the second lens element 2 are both aspheric.
The third lens element 3 has a positive refractive index, and an object-side surface 31 of the third lens element 3 is a convex surface and an image-side surface 32 of the third lens element 3 is a convex surface.
The fourth lens element 4 has a negative refractive index, and the object-side surface 41 of the fourth lens element 4 is concave, and the image-side surface 42 of the fourth lens element 4 is concave, but not limited thereto.
The object-side surface 41 and the image-side surface 42 of the fourth lens element 4 are both aspheric.
The fifth lens element 5 has a positive refractive index, the object-side surface 51 of the fifth lens element 5 is convex, the image-side surface 52 of the fifth lens element 5 is convex, and both the object-side surface 51 and the image-side surface 52 of the fifth lens element 5 are aspheric.
The first lens 1 and the third lens 3 are made of glass materials, and the second lens 2, the fourth lens 4 and the fifth lens 5 are made of plastic materials.
The temperature coefficient of refractive index of the third lens 3 is negative.
In this embodiment, the diaphragm 6 is disposed between the second lens 2 and the third lens 3, so as to improve the overall performance, and of course, in other embodiments, the diaphragm 6 may be disposed at other suitable positions.
In this embodiment, the first lens 1 and the second lens 2 are connected by a lens barrel bearing platform, and the fourth lens 4 and the fifth lens 5 are directly connected by a lens edge.
The detailed optical data of this embodiment are shown in Table 1-1.
Table 1-1 detailed optical data for example one
In this embodiment, the object-side surface 21, the object-side surface 41, the object-side surface 51, the image-side surface 22, the image-side surface 42, and the image-side surface 52 are defined by the following aspheric curve formulas:
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: curvature of aspheric vertex (thevertexcurvature);
k: cone coefficient (Conicconstant);
rn: normalized radius (normalizationradius (nradius));
u:r/rn;
am: mth order QconCoefficient (isthem)thQconcoefficient);
Qm con: mth order QconPolynomial (then)thQconpolynomial);
For details of parameters of each aspheric surface, please refer to the following table:
please refer to table 6 for the values of the conditional expressions related to this embodiment.
The MTF graph of the present embodiment is shown in fig. 2 and 7 in detail, and it can be seen that under the visible light condition, the MTF value of the spatial frequency 167lp/mm is greater than 0.35, which can reach five million pixels, and under the infrared light condition, the MTF value of the spatial frequency 167lp/mm is also greater than 0.3, which ensures the imaging quality and meets the requirement of the image definition; referring to the defocus graphs of fig. 3 and 8, it can be seen that when the infrared imaging is switched, the IRshift (infrared shift) is less than 5 μm, and the day and night confocality is good; referring to fig. 4, it can be seen that the lateral chromatic aberration is corrected well; referring to fig. 5, it can be seen that the relative illuminance of the imaging edge is large, greater than 50%; referring to fig. 6, it can be seen that the aberration is small and the imaging quality is good.
In the specific embodiment, the F-Theta distortion is less than-5%, the image edge compression amount is small, the pixel values distributed by the edge unit angle are more, and the loss of the angle of the edge of the view field is small.
In the embodiment, temperature compensation is considered in design, and when the temperature compensation is used in a temperature range of-40 ℃ to 70 ℃, an image picture is not distorted.
In the specific embodiment, the focal length f of the glass-plastic mixed infrared confocal lens is 3.1 mm; f-number FNO 1.8; the field angle FOV is 127 °; the size of the image surface is 1/2.7 inches; the distance TTL between the object side surface 11 of the first lens element 1 and the image forming surface 8 on the optical axis I is 22.50 mm.
Example two
As shown in fig. 9, the lens elements of this embodiment have the same surface roughness and refractive index as those of the first embodiment, and only the optical parameters such as the curvature radius and the lens thickness of the surface of each lens element are different.
The detailed optical data of this embodiment is shown in Table 2-1.
TABLE 2-1 detailed optical data for example two
For the detailed data of the parameters of each aspheric surface of this embodiment, refer to the following table:
surface of | K | a4 | a6 | a8 | a10 | a12 | a14 | a16 |
21 | 0.96 | -3.101E-04 | 7.117E-05 | -2.228E-06 | 5.644E-08 | 5.696E-05 | -4.337E-09 | |
22 | -0.22 | 7.014E-04 | 7.564E-04 | -3.100E-05 | 1.173E-06 | -3.080E-08 | -2.183E-09 | |
41 | -48.26 | -2.852E-02 | 1.107E-02 | -3.686E-03 | 7.682E-04 | -8.953E-05 | 4.355E-06 | |
42 | -5.46 | -9.024E-03 | 6.251E-03 | -6.118E-03 | 4.094E-04 | -4.307E-05 | 1.812E-06 | -7.139E-08 |
51 | -7.70 | 2.223E-04 | 1.701E-03 | -4.845E-04 | 8.813E-05 | -9.948E-06 | 1.366E-07 | 1.507E-08 |
52 | -12.84 | -9.757E-03 | 1.334E-03 | -1.473E-04 | 1.450E-05 | -1.690E-06 | 3.338E-07 | -1.853E-08 |
Please refer to table 6 for the values of the conditional expressions related to this embodiment.
The MTF graph of the present embodiment is shown in fig. 10 and 15 in detail, and it can be seen that under the visible light condition, the MTF value of the spatial frequency 167lp/mm is greater than 0.35, which can reach five million pixels, and under the infrared light condition, the MTF value of the spatial frequency 167lp/mm is also greater than 0.3, which ensures the imaging quality and meets the requirement of the image definition; referring to fig. 11 and 16, it can be seen that when the infrared imaging is switched, the IRshift (infrared shift) is less than 5 μm, and the day and night confocality is good; referring to fig. 12, it can be seen that the lateral chromatic aberration is corrected well; referring to fig. 13, it can be seen that the relative illuminance of the imaging edge is large, greater than 50%; referring to fig. 14, it can be seen that the aberration is small and the imaging quality is good.
In the specific embodiment, the F-Theta distortion is less than-5%, the image edge compression amount is small, the pixel values distributed by the edge unit angle are more, and the loss of the angle of the edge of the view field is small.
In the embodiment, temperature compensation is considered in design, and when the temperature compensation is used in a temperature range of-40 ℃ to 70 ℃, an image picture is not distorted.
In the specific embodiment, the focal length f of the glass-plastic mixed infrared confocal lens is 3.1 mm; f-number FNO 1.8; the field angle FOV is 127 °; the size of the image surface is 1/2.7 inches; the distance TTL between the object side surface 11 of the first lens element 1 and the image forming surface 8 on the optical axis I is 22.50 mm.
EXAMPLE III
As shown in fig. 17, the lens elements of this embodiment have the same surface roughness and refractive index as those of the first embodiment, and only the optical parameters such as the curvature radius of the surface of each lens element and the lens thickness are different.
The detailed optical data of this embodiment is shown in Table 3-1.
TABLE 3-1 detailed optical data for EXAMPLE III
For the detailed data of the parameters of each aspheric surface of this embodiment, refer to the following table:
surface of | K | a4 | a6 | a8 | a10 | a12 | a14 | a16 |
21 | 0.97 | -4.140E-04 | 8.698E-05 | -4.474E-06 | -5.311E-08 | 1.130E-07 | -8.528E-09 | |
22 | -0.26 | 6.752E-04 | 6.698E-05 | -1.078E-05 | 1.336E-06 | -7.375E-08 | 2.313E-10 | |
41 | -41.66 | -2.848E-02 | 1.108E-02 | -5.693E-03 | 7.670E-04 | -8.937E-05 | 4.365E-06 | |
42 | -5.33 | -9.237E-03 | 6.241E-03 | -2.119E-03 | 4.093E-04 | -4.337E-05 | 1.852E-04 | -1.382E-05 |
51 | -7.59 | 6.254E-05 | 6.696E-03 | -4.856E-04 | 8.785E-05 | -7.956E-06 | 1.413E-07 | 1.554E-08 |
52 | -13.55 | -1.088E-03 | 1.309E-03 | -1.451E-04 | 3.460E-05 | -1.672E-06 | 3.360E-07 | -1.792E-08 |
Please refer to table 6 for the values of the conditional expressions related to this embodiment.
The MTF graph of the present embodiment is shown in fig. 18 and 23 in detail, and it can be seen that under the visible light condition, the MTF value of the spatial frequency 167lp/mm is greater than 0.35, which can reach five million pixels, and under the infrared light condition, the MTF value of the spatial frequency 167lp/mm is also greater than 0.3, which ensures the imaging quality and meets the requirement of the image definition; referring to fig. 19 and 24, it can be seen that when the infrared imaging is switched, the IRshift (infrared shift) is less than 5 μm, and the day and night confocality is good; referring to fig. 20, it can be seen that the lateral chromatic aberration is corrected well; referring to fig. 21, it can be seen that the relative illuminance of the imaging edge is large, greater than 50%; referring to fig. 22, it can be seen that the aberration is small and the imaging quality is good.
In the specific embodiment, the F-Theta distortion is less than-5%, the image edge compression amount is small, the pixel values distributed by the edge unit angle are more, and the loss of the angle of the edge of the view field is small.
In the embodiment, temperature compensation is considered in design, and when the temperature compensation is used in a temperature range of-40 ℃ to 70 ℃, an image picture is not distorted.
In the specific embodiment, the focal length f of the glass-plastic mixed infrared confocal lens is 3.1 mm; f-number FNO 1.8; the field angle FOV is 127 °; the size of the image surface is 1/2.7 inches; the distance TTL between the object side surface 11 of the first lens element 1 and the image forming surface 8 on the optical axis I is 22.50 mm.
Example four
As shown in fig. 25, the lens elements of this embodiment have the same surface roughness and refractive index as those of the first embodiment, and only the optical parameters such as the curvature radius and the lens thickness of the surface of each lens element are different.
The detailed optical data of this embodiment is shown in Table 4-1.
TABLE 4-1 detailed optical data for example four
For the detailed data of the parameters of each aspheric surface of this embodiment, refer to the following table:
surface of | K | a4 | a6 | a8 | a10 | a12 | a14 | a16 |
21 | -0.13 | -5.248E-04 | -2.009E-04 | 1.095E-04 | -2.610E-05 | 3.031E-06 | -1.382E-05 | |
22 | -0.33 | 3.118E-04 | 1.530E-04 | -3.573E-05 | 3.462E-06 | 5.767E-08 | -2.285E-08 | |
41 | -6.96 | -2.844E-02 | 9.852E-03 | -3.314E-03 | 5.215E-04 | -8.821E-05 | 4.506E-06 | |
42 | -4.68 | -8.965E-03 | 6.002E-03 | -2.091E-03 | 4.136E-04 | -4.459E-05 | 1.952E-06 | -3.314E-03 |
51 | -7.28 | -3.545E-04 | 1.851E-03 | -5.409E-04 | 8.921E-05 | -6.753E-06 | -8.283E-08 | 2.980E-08 |
52 | -9.85 | -7.157E-03 | 1.227E-03 | -1.694E-04 | 2.900E-05 | -2.261E-06 | 6.125E-08 | 7.544E-09 |
Please refer to table 6 for the values of the conditional expressions related to this embodiment.
The MTF graph of the present embodiment is shown in fig. 26 and 31 in detail, and it can be seen that under the visible light condition, the MTF value of the spatial frequency 167lp/mm is greater than 0.35, which can reach five million pixels, and under the infrared light condition, the MTF value of the spatial frequency 167lp/mm is also greater than 0.3, which ensures the imaging quality and meets the requirement of the image definition; referring to the defocus graphs of fig. 27 and 32, it can be seen that when the infrared imaging is switched, the IRshift (infrared shift) is less than 5 μm, and the day and night confocality is good; referring to fig. 28, it can be seen that the lateral chromatic aberration is corrected well; referring to fig. 29, it can be seen that the relative illuminance at the imaging edge is large, greater than 50%; referring to fig. 30, it can be seen that the aberration is small and the imaging quality is good.
In the specific embodiment, the F-Theta distortion is less than-5%, the image edge compression amount is small, the pixel values distributed by the edge unit angle are more, and the loss of the angle of the edge of the view field is small.
In the embodiment, temperature compensation is considered in design, and when the temperature compensation is used in a temperature range of-40 ℃ to 70 ℃, an image picture is not distorted.
In the specific embodiment, the focal length f of the glass-plastic mixed infrared confocal lens is 3.1 mm; f-number FNO 1.8; the field angle FOV is 127 °; the size of the image surface is 1/2.7 inches; the distance TTL between the object side surface 11 of the first lens element 1 and the image forming surface 8 on the optical axis I is 22.50 mm.
EXAMPLE five
As shown in fig. 33, the lens elements of this embodiment have the same surface roughness and refractive index as those of the first embodiment, and only the optical parameters such as the curvature radius and the lens thickness of the surface of each lens element are different.
The detailed optical data of this embodiment is shown in Table 5-1.
TABLE 5-1 detailed optical data for EXAMPLE V
For the detailed data of the parameters of each aspheric surface of this embodiment, refer to the following table:
please refer to table 6 for the values of the conditional expressions related to this embodiment.
The MTF graph of the present embodiment is shown in fig. 34 and 39 in detail, and it can be seen that under the visible light condition, the MTF value of the spatial frequency 167lp/mm is greater than 0.35, which can reach five million pixels, and under the infrared light condition, the MTF value of the spatial frequency 167lp/mm is also greater than 0.3, which ensures the imaging quality and meets the requirement of the image definition; referring to fig. 35 and 40, it can be seen that when the infrared imaging is switched, the IRshift (infrared shift) is less than 5 μm, and the day and night confocality is good; referring to fig. 36, it can be seen that the chromatic aberration is corrected well; referring to fig. 37, it can be seen that the relative illuminance of the imaging edge is large, greater than 50%; referring to fig. 38, it can be seen that the aberration is small and the imaging quality is good.
In the specific embodiment, the F-Theta distortion is less than-5%, the image edge compression amount is small, the pixel values distributed by the edge unit angle are more, and the loss of the angle of the edge of the view field is small.
In the embodiment, temperature compensation is considered in design, and when the temperature compensation is used in a temperature range of-40 ℃ to 70 ℃, an image picture is not distorted.
In the specific embodiment, the focal length f of the glass-plastic mixed infrared confocal lens is 3.1 mm; f-number FNO 1.8; the field angle FOV is 127 °; the size of the image surface is 1/2.7 inches; the distance TTL between the object side surface 11 of the first lens element 1 and the image forming surface 8 on the optical axis I is 22.50 mm.
TABLE 6 values of relevant important parameters for five embodiments of the invention
First embodiment | Second embodiment | Third embodiment | Fourth embodiment | Fifth embodiment | |
f1 | -5.41 | -5.37 | -5.26 | -5.18 | -5.21 |
f2 | 22.36 | 22.70 | 22.86 | 21.23 | 22.10 |
f3 | 7.61 | 7.49 | 7.55 | 7.16 | 7.19 |
f4 | -4.81 | -4.79 | -4.82 | -4.71 | -4.71 |
f5 | 4.55 | 4.58 | 4.52 | 4.57 | 4.53 |
f | 3.1 | 3.1 | 3.1 | 3.1 | 3.1 |
f2/f | 7.21 | 7.32 | 7.37 | 6.85 | 7.13 |
f3/f | 2.45 | 2.42 | 2.44 | 2.31 | 2.32 |
f5/f | 1.47 | 1.48 | 1.46 | 1.47 | 1.46 |
D11 | 8.979 | 8.848 | 8.722 | 8.791 | 9.096 |
R11 | 15.012 | 14.294 | 14.155 | 14.502 | 14.708 |
D11/R11 | 0.60 | 0.62 | 0.62 | 0.61 | 0.62 |
D31 | 6.000 | 6.000 | 7.000 | 7.000 | 7.000 |
R31 | 13.144 | 13.397 | 13.783 | 14.457 | 13.060 |
D31/R31 | 0.46 | 0.45 | 0.51 | 0.48 | 0.54 |
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 (10)
1. The utility model provides a glass is moulded and is mixed infrared confocal camera lens which characterized in that: the lens comprises a first lens, a second lens, a third lens, a fourth lens, a fifth lens and a fourth lens, wherein the first lens, the second lens and the fifth lens are arranged in sequence from the object side to the image side along an optical axis; the first lens, the second lens, the third lens and the fourth lens are respectively arranged on the object side and the image side, and the object side faces towards the object side and enables the imaging light rays to pass through;
the first lens element with negative refractive index has a convex object-side surface and a concave image-side surface;
the second lens has positive refractive index;
the third lens element with positive refractive index has a convex object-side surface and a convex image-side surface;
the fourth lens element has negative refractive index;
the fifth lens element with positive refractive index has a convex object-side surface and a convex image-side surface;
the first lens and the third lens are both glass spherical lenses, and the second lens, the fourth lens and the fifth lens are all plastic aspheric lenses;
the temperature coefficient of the refractive index of the third lens is a negative value;
the glass-plastic mixed infrared confocal lens is provided with the lenses with the refractive index only from the first lens to the fifth lens.
2. The glass-plastic mixed infrared confocal lens of claim 1, wherein the glass-plastic mixed infrared confocal lens further satisfies: nd1>1.75, where nd1 is the refractive index of the first lens.
3. The glass-plastic mixed infrared confocal lens of claim 1, wherein the glass-plastic mixed infrared confocal lens further satisfies: nd2>1.6, nd4>1.6, where nd2 is the refractive index of the second lens and nd4 is the refractive index of the fourth lens.
4. The glass-plastic hybrid infrared confocal lens of claim 1, characterized in that: the second lens, the fourth lens and the fifth lens are all high-order even-order aspheric lenses.
5. The glass-plastic hybrid infrared confocal lens of claim 1, characterized in that: the first lens and the second lens are connected by a lens cone bearing platform.
6. The glass-plastic hybrid infrared confocal lens of claim 1, characterized in that: the fourth lens is directly abutted and jointed with the edge of the fifth lens.
7. The glass-plastic mixed infrared confocal lens of claim 1, wherein the glass-plastic mixed infrared confocal lens further satisfies: 6.5< f2/f <9, 1.5< f3/f <3 and 1< f5/f <2, wherein f is the focal length of the glass-plastic hybrid infrared confocal lens, f2 is the focal length of the second lens, f3 is the focal length of the third lens, and f5 is the focal length of the fifth lens.
8. The glass-plastic mixed infrared confocal lens of claim 1, wherein the glass-plastic mixed infrared confocal lens further satisfies: -7mm < f1< -4mm, 21mm < f2<23mm, 6mm < f3<8mm, -5mm < f4< -3mm and 3mm < f5<5mm, wherein f1, f2, f3, f4, f5 are the focal lengths of the first lens, the second lens, the third lens, the fourth lens and the fifth lens, respectively.
9. The glass-plastic mixed infrared confocal lens of claim 1, wherein the glass-plastic mixed infrared confocal lens further satisfies: 14mm < R11<16mm, 2mm < R12<4mm, -6mm < R21< -4mm, -6mm < R22< -4mm, 13mm < R31<16mm, -7mm < R32< -5mm, 10mm < R41<13mm, 2mm < R42<4mm, 3mm < R51<5mm, and-6 mm < R52< -4mm, wherein R11, R21, R31, R41, and R51 are radii of curvature of object sides of the first lens, the second lens, the third lens, the fourth lens, and the fifth lens, and R12, R22, R32, R42, and R52 are radii of curvature of image sides of the first lens, the second lens, the third lens, the fourth lens, and the fifth lens, respectively.
10. The glass-plastic mixed infrared confocal lens of claim 1, wherein the glass-plastic mixed infrared confocal lens further satisfies: 0.3< D11/R11<0.7 and 0.3< D31/R31<0.7, wherein D11 and D31 are clear apertures of object-side surfaces of the first lens and the third lens, respectively, and R11 and R31 are radii of curvature of the object-side surfaces of the first lens and the third lens, respectively.
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