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WO2021128141A1 - Lentille optique de caméra - Google Patents

Lentille optique de caméra Download PDF

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Publication number
WO2021128141A1
WO2021128141A1 PCT/CN2019/128596 CN2019128596W WO2021128141A1 WO 2021128141 A1 WO2021128141 A1 WO 2021128141A1 CN 2019128596 W CN2019128596 W CN 2019128596W WO 2021128141 A1 WO2021128141 A1 WO 2021128141A1
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Prior art keywords
lens
imaging optical
ttl
optical lens
curvature
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PCT/CN2019/128596
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English (en)
Chinese (zh)
Inventor
生沼健司
张磊
崔元善
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AAC Optics Changzhou Co Ltd
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AAC Optics Changzhou Co Ltd
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Priority to PCT/CN2019/128596 priority Critical patent/WO2021128141A1/fr
Publication of WO2021128141A1 publication Critical patent/WO2021128141A1/fr
Anticipated expiration legal-status Critical
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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

Definitions

  • the present invention relates to the field of optical lenses, in particular to an imaging optical lens suitable for portable terminal equipment such as smart phones and digital cameras, as well as imaging devices such as monitors and PC lenses.
  • the photosensitive devices of general photographic lenses are nothing more than photosensitive coupled devices (CCD) or complementary metal oxide semiconductor devices (Complementary Metal).
  • CCD photosensitive coupled devices
  • CMOS Sensor complementary metal oxide semiconductor devices
  • the lenses traditionally mounted on mobile phone cameras often adopt a three-element, four-element, five-element or even six-element lens structure.
  • the seven-element lens structure gradually appears in the lens design.
  • the seven-element lens has good optical performance, its optical power, lens spacing and lens shape settings are still unreasonable, resulting in the lens structure having good optical performance while being unable to meet the requirements of ultra-thinness. , Wide-angle design requirements.
  • the object of the present invention is to provide an imaging optical lens, which has good optical performance and meets the design requirements of ultra-thin and wide-angle.
  • the present invention provides an imaging optical lens which sequentially includes from the object side to the image side: a first lens with negative refractive power, a second lens with positive refractive power, and a first lens with positive refractive power.
  • a first lens with negative refractive power a second lens with positive refractive power
  • a first lens with positive refractive power a third lens with positive refractive power.
  • the maximum field angle of the imaging optical lens is FOV
  • the focal length of the second lens is f2
  • the focal length of the imaging optical lens is f
  • the axial thickness of the third lens is d5
  • the seventh lens The on-axis thickness of is d13
  • the dispersion coefficient of the third lens is v3
  • the dispersion coefficient of the fifth lens is v5, which satisfies the following relationship:
  • the image side surface of the first lens is concave on the paraxial;
  • the focal length of the first lens is f1
  • the radius of curvature of the object side surface of the first lens is R1
  • the radius of curvature of the image side surface of the first lens is R2
  • the on-axis thickness of the first lens is d1
  • the total optical length of the imaging optical lens is TTL, and the following relationship is satisfied:
  • the imaging optical lens satisfies the following relationship:
  • the radius of curvature of the object side surface of the second lens is R3
  • the radius of curvature of the image side surface of the second lens is R4
  • the axial thickness of the second lens is d3
  • the total optical length of the imaging optical lens is TTL, satisfies the following relationship:
  • the imaging optical lens satisfies the following relationship:
  • the object side surface of the third lens is convex on the paraxial axis, and the image side surface is convex on the paraxial axis;
  • the focal length of the third lens is f3
  • the radius of curvature of the object side of the third lens is R5
  • the radius of curvature of the image side of the third lens is R6, and the total optical length of the imaging optical lens is TTL, which satisfies the following relationship formula:
  • the imaging optical lens satisfies the following relationship:
  • the focal length of the fourth lens is f4
  • the radius of curvature of the object side of the fourth lens is R7
  • the radius of curvature of the image side of the fourth lens is R8,
  • the on-axis thickness of the fourth lens is d7
  • the total optical length of the camera optical lens is TTL, which satisfies the following relationship:
  • the imaging optical lens satisfies the following relationship:
  • the object side surface of the fifth lens is concave on the paraxial axis, and the image side surface is convex on the paraxial axis;
  • the focal length of the fifth lens is f5
  • the radius of curvature of the object side of the fifth lens is R9
  • the radius of curvature of the image side of the fifth lens is R10
  • the axial thickness of the fifth lens is d9
  • the total optical length of the camera optical lens is TTL, which satisfies the following relationship:
  • the imaging optical lens satisfies the following relationship:
  • the object side of the sixth lens is convex on the paraxial axis
  • the focal length of the sixth lens is f6
  • the radius of curvature of the object side of the sixth lens is R11
  • the radius of curvature of the image side of the sixth lens is R12
  • the on-axis thickness of the sixth lens is d11
  • the total optical length of the imaging optical lens is TTL, which satisfies the following relationship:
  • the imaging optical lens satisfies the following relationship:
  • the image side surface of the seventh lens is concave on the paraxial axis, and the object side surface is convex on the paraxial axis;
  • the focal length of the seventh lens is f7
  • the radius of curvature of the object side of the seventh lens is R13
  • the radius of curvature of the image side of the seventh lens is R14
  • the total optical length of the imaging optical lens is TTL
  • the imaging optical lens satisfies the following relationship:
  • the total optical length TTL of the imaging optical lens is less than or equal to 7.37 mm.
  • the total optical length TTL of the imaging optical lens is less than or equal to 7.04 mm.
  • the aperture F number of the imaging optical lens is less than or equal to 2.68.
  • the aperture F number of the imaging optical lens is less than or equal to 2.63.
  • the imaging optical lens according to the present invention has good optical performance, wide-angle and ultra-thin characteristics, and is especially suitable for mobile phone camera lens assemblies composed of high-pixel CCD, CMOS and other imaging elements And WEB camera lens.
  • FIG. 1 is a schematic diagram of the structure of an imaging optical lens of the first embodiment
  • FIG. 2 is a schematic diagram of axial aberration of the imaging optical lens shown in FIG. 1;
  • FIG. 3 is a schematic diagram of the chromatic aberration of magnification of the imaging optical lens shown in FIG. 1;
  • FIG. 4 is a schematic diagram of field curvature and distortion of the imaging optical lens shown in FIG. 1;
  • FIG. 5 is a schematic diagram of the structure of the imaging optical lens of the second embodiment
  • FIG. 6 is a schematic diagram of axial aberration of the imaging optical lens shown in FIG. 5;
  • FIG. 7 is a schematic diagram of the chromatic aberration of magnification of the imaging optical lens shown in FIG. 5;
  • FIG. 8 is a schematic diagram of field curvature and distortion of the imaging optical lens shown in FIG. 5;
  • FIG. 9 is a schematic diagram of the structure of the imaging optical lens of the third embodiment.
  • FIG. 10 is a schematic diagram of axial aberration of the imaging optical lens shown in FIG. 9;
  • FIG. 11 is a schematic diagram of the chromatic aberration of magnification of the imaging optical lens shown in FIG. 9;
  • FIG. 12 is a schematic diagram of field curvature and distortion of the imaging optical lens shown in FIG. 9.
  • FIG. 1 shows an imaging optical lens 10 according to a first embodiment of the present invention.
  • the imaging optical lens 10 includes seven lenses. Specifically, the imaging optical lens 10 includes in order from the object side to the image side: a first lens L1 with a negative refractive power, an aperture S1, a second lens L2 with a positive refractive power, and a third lens with a positive refractive power.
  • An optical element such as an optical filter GF may be provided between the seventh lens L7 and the image plane Si.
  • the first lens L1 is made of plastic
  • the second lens L2 is made of plastic
  • the third lens L3 is made of plastic
  • the fourth lens L4 is made of plastic
  • the fifth lens L5 is made of plastic
  • the sixth lens L6 is made of plastic
  • the seventh lens is made of plastic.
  • the lens L7 is made of plastic.
  • the maximum angle of view of the imaging optical lens 10 is defined as FOV, which satisfies the following relationship 100.00° ⁇ FOV ⁇ 135.00°. Within the range of the maximum angle of view of the imaging optical lens 10 that satisfies the relational formula, ultra-wide-angle imaging can be achieved, and user experience can be improved.
  • the focal length of the second lens L2 is defined as f2, and the focal length of the imaging optical lens 10 is defined as f, and the following relationship is satisfied: 1.00 ⁇ f2/f ⁇ 3.00.
  • the on-axis thickness of the third lens L3 is defined as d5, and the on-axis thickness of the seventh lens L7 is defined as d13, and the following relationship is satisfied: 1.50 ⁇ d5/d13 ⁇ 3.00.
  • the ratio of the on-axis thickness of the third lens L3 to the on-axis thickness of the seventh lens L7 is specified. When the ratio is within the range, it is beneficial to the development of the lens to a wider angle.
  • the dispersion coefficient of the third lens L3 is defined as v3, and the dispersion coefficient of the fifth lens L5 is defined as v5, and the following relationship is satisfied: 2.00 ⁇ v3-v5 ⁇ 20.00.
  • the difference between the dispersion coefficients of the third lens L3 and the fifth lens L5 is specified. Within the range, it can effectively correct the dispersion of the imaging optical lens, improve the sharpness of the imaging, close to the true color of the subject, and improve the imaging quality.
  • the first lens L1 has a negative refractive power, and its image side surface is concave on the paraxial axis.
  • the focal length of the first lens L1 is f1, which satisfies the following relationship: -11.87 ⁇ f1/f ⁇ -1.04, which specifies the ratio of the negative refractive power of the first lens L1 to the overall focal length.
  • the first lens L1 has an appropriate negative refractive power, which is beneficial to reduce system aberrations, and at the same time, is beneficial to the development of ultra-thin and wide-angle lenses.
  • the curvature radius R1 of the object side surface of the first lens L1 and the curvature radius R2 of the image side surface of the first lens L1 satisfy the following relationship: 0.15 ⁇ (R1+R2)/(R1-R2) ⁇ 12.07, reasonable control of the first lens L1
  • the shape enables the first lens L1 to effectively correct the spherical aberration of the system.
  • the axial thickness of the first lens L1 is d1
  • the total optical length of the imaging optical lens is TTL, which satisfies the following relationship: 0.02 ⁇ d1/TTL ⁇ 0.08, which is conducive to achieving ultra-thinness.
  • the curvature radius R3 of the object side surface of the second lens L2 is defined, and the curvature radius R4 of the image side surface of the second lens L2 is defined to satisfy the following relationship: -12.96 ⁇ (R3+R4)/(R3-R4) ⁇ 3.63,
  • the shape of the second lens L2 is specified.
  • the lens is within the range, as the lens becomes ultra-thin and wide-angle, it is beneficial to correct the problem of axial chromatic aberration.
  • the on-axis thickness of the second lens L2 is d3, and the total optical length of the imaging optical lens is TTL, which satisfies the following relationship: 0.03 ⁇ d3/TTL ⁇ 0.14, which is conducive to achieving ultra-thinness.
  • the object side surface of the third lens L3 is convex on the paraxial axis, and its side surface is convex on the paraxial axis.
  • the focal length of the third lens L3 is f3, and satisfies the following relational expression: 0.51 ⁇ f3/f ⁇ 9.17.
  • the system has better imaging quality and lower sensitivity.
  • the curvature radius R5 of the object side surface of the third lens L3 and the curvature radius R6 of the image side surface of the third lens L3 satisfy the following relationship: -0.66 ⁇ (R5+R6)/(R5-R6) ⁇ 0.80, which can effectively control the third lens
  • the shape of L3 is conducive to the molding of the third lens L3.
  • the degree of deflection of the light passing through the lens can be eased, and aberrations can be effectively reduced.
  • the axial thickness of the third lens L3 is d5, and the total optical length of the imaging optical lens is TTL, which satisfies the following relationship: 0.06 ⁇ d5/TTL ⁇ 0.20, which is conducive to achieving ultra-thinness.
  • the focal length f4 of the fourth lens L4 satisfies the following relational expression: -6.54 ⁇ f4/f ⁇ -0.82.
  • the reasonable distribution of optical power enables the system to have better imaging quality and lower sensitivity.
  • the curvature radius R7 of the object side surface of the fourth lens L4 and the curvature radius R8 of the image side surface of the fourth lens L4 satisfy the following relationship: -5.54 ⁇ (R7+R8)/(R7-R8) ⁇ 2.95, the fourth lens is specified
  • the shape of L4 is within the range, with the development of ultra-thin and wide-angle, it is helpful to correct the aberration of the off-axis angle of view.
  • the axial thickness of the fourth lens L4 is d7, and the total optical length of the imaging optical lens is TTL, which satisfies the following relationship: 0.02 ⁇ d7/TTL ⁇ 0.07, which is conducive to achieving ultra-thinness.
  • the object side surface of the fifth lens L5 is concave on the paraxial axis, and its side surface is convex on the paraxial axis.
  • the focal length f5 of the fifth lens L5 satisfies the following relationship: -7.42 ⁇ f5/f ⁇ 1.31.
  • the limitation of the fifth lens L5 can effectively smooth the light angle of the imaging lens and reduce the tolerance sensitivity.
  • the curvature radius R9 of the object side surface of the fifth lens L5 and the curvature radius R10 of the image side surface of the fifth lens L5 satisfy the following relationship: -2.20 ⁇ (R9+R10)/(R9-R10) ⁇ 3.99, the fifth lens is specified
  • the shape of L5 is within the range of conditions, with the development of ultra-thin and wide-angle, it is conducive to correcting the aberration of the off-axis angle of view.
  • the on-axis thickness of the fifth lens L5 is d9, and the total optical length of the imaging optical lens is TTL, which satisfies the following relationship: 0.05 ⁇ d9/TTL ⁇ 0.30, which is conducive to achieving ultra-thinness.
  • the focal length f6 of the sixth lens L6 satisfies the following relational expression: -2144.75 ⁇ f6/f ⁇ 1.14.
  • the reasonable distribution of optical power enables the system to have better imaging quality and lower sensitivity.
  • the curvature radius R11 of the object side surface of the sixth lens L6 and the curvature radius R12 of the image side surface of the sixth lens L6 satisfy the following relationship: 0.46 ⁇ (R11+R12)/(R11-R12) ⁇ 81.92, and the sixth lens L6 is specified
  • the shape is within the range of conditions, with the development of ultra-thin and wide-angle, it is helpful to correct the aberration of the off-axis angle of view.
  • the on-axis thickness of the sixth lens L6 is d11, and the total optical length of the imaging optical lens is TTL, which satisfies the following relationship: 0.04 ⁇ d11/TTL ⁇ 0.25, which is conducive to achieving ultra-thinness.
  • 0.07 ⁇ d11/TTL ⁇ 0.20.
  • the mirror side surface of the seventh lens L7 is concave on the paraxial axis.
  • the focal length f7 of the seventh lens L7 satisfies the following relational expression: -2.02 ⁇ f7/f ⁇ 45.76.
  • the system has better imaging quality and lower sensitivity.
  • the curvature radius of the image side surface of the seventh lens is R14, and the on-axis thickness of the seventh lens is d13, which satisfies the following relationship: -3.34 ⁇ (R13+R14)/(R13-R14) ⁇ 3.63, which is
  • -3.34 ⁇ (R13+R14)/(R13-R14) ⁇ 3.63 which is
  • the shape of the sixth lens L6 is within the range of conditions, with the development of ultra-thin and wide-angle, it is beneficial to correct the aberration of the off-axis angle of view.
  • the on-axis thickness of the seventh lens L7 is d13, and the total optical length of the imaging optical lens is TTL, which satisfies the following relationship: 0.02 ⁇ d13/TTL ⁇ 0.12, which is conducive to achieving ultra-thinness.
  • the total optical length TTL of the imaging optical lens 10 is less than or equal to 7.37 mm, which is beneficial to realize ultra-thinness.
  • the total optical length TTL of the imaging optical lens 10 is less than or equal to 7.04 mm.
  • the aperture F number of the imaging optical lens 10 is less than or equal to 2.68. Large aperture, good imaging performance. Preferably, the aperture F number of the imaging optical lens 10 is less than or equal to 2.63.
  • the overall optical length TTL of the overall imaging optical lens 10 can be shortened as much as possible, and the characteristics of miniaturization can be maintained.
  • the imaging optical lens 10 realizes the design requirements of wide-angle and ultra-thin design while having good optical imaging performance; according to the characteristics of the imaging optical lens 10, the imaging optical lens 10
  • the lens 10 is particularly suitable for a mobile phone camera lens assembly and a WEB camera lens composed of high-resolution CCD, CMOS, and other imaging elements.
  • the imaging optical lens 10 of the present invention will be described below with an example.
  • the symbols described in each example are as follows.
  • the unit of focal length, distance on axis, radius of curvature, thickness on axis, position of inflection point, and position of stagnation point is mm.
  • TTL total optical length (the on-axis distance from the object side of the first lens L1 to the image plane Si), the unit is mm;
  • the object side and/or the image side of the lens can also be provided with inflection points and/or stagnation points to meet high-quality imaging requirements.
  • inflection points and/or stagnation points for specific implementations, refer to the following.
  • Table 1 and Table 2 show design data of the imaging optical lens 10 according to the first embodiment of the present invention.
  • R The radius of curvature of the optical surface, and the radius of curvature of the center of the lens
  • R1 the radius of curvature of the object side surface of the first lens L1;
  • R2 the radius of curvature of the image side surface of the first lens L1;
  • R3 the radius of curvature of the object side surface of the second lens L2;
  • R4 the radius of curvature of the image side surface of the second lens L2;
  • R5 the radius of curvature of the object side surface of the third lens L3;
  • R6 the radius of curvature of the image side surface of the third lens L3;
  • R7 the radius of curvature of the object side of the fourth lens L4;
  • R8 the radius of curvature of the image side surface of the fourth lens L4;
  • R9 the radius of curvature of the object side surface of the fifth lens L5;
  • R10 the radius of curvature of the image side surface of the fifth lens L5;
  • R11 the radius of curvature of the object side surface of the sixth lens L6;
  • R12 the radius of curvature of the image side surface of the sixth lens L6;
  • R13 the radius of curvature of the object side surface of the seventh lens L7;
  • R14 the radius of curvature of the image side surface of the seventh lens L7;
  • R15 the radius of curvature of the object side of the optical filter GF
  • R16 the radius of curvature of the image side surface of the optical filter GF
  • d0 the on-axis distance from the aperture S1 to the object side of the first lens L1;
  • d2 the on-axis distance from the image side surface of the first lens L1 to the object side surface of the second lens L2;
  • d4 the on-axis distance from the image side surface of the second lens L2 to the object side surface of the third lens L3;
  • d6 the on-axis distance from the image side surface of the third lens L3 to the object side surface of the fourth lens L4;
  • d10 the on-axis distance from the image side surface of the fifth lens L5 to the object side surface of the sixth lens L6;
  • d11 the on-axis thickness of the sixth lens L6;
  • d12 the on-axis distance from the image side surface of the sixth lens L6 to the object side surface of the seventh lens L7;
  • d14 the on-axis distance from the image side surface of the seventh lens L7 to the object side surface of the optical filter GF;
  • d15 the axial thickness of the optical filter GF
  • d16 the on-axis distance from the image side surface of the optical filter GF to the image surface
  • nd refractive index of d-line
  • nd1 the refractive index of the d-line of the first lens L1;
  • nd2 the refractive index of the d-line of the second lens L2;
  • nd3 the refractive index of the d-line of the third lens L3;
  • nd4 the refractive index of the d-line of the fourth lens L4;
  • nd5 the refractive index of the d-line of the fifth lens L5;
  • nd6 the refractive index of the d-line of the sixth lens L6;
  • ndg the refractive index of the d-line of the optical filter GF
  • ⁇ 1 the dispersion coefficient of the first lens L1;
  • ⁇ 2 the dispersion coefficient of the second lens L2
  • ⁇ 3 the dispersion coefficient of the third lens L3
  • ⁇ 4 the dispersion coefficient of the fourth lens L4
  • ⁇ 5 the dispersion coefficient of the fifth lens L5
  • ⁇ 6 the dispersion coefficient of the sixth lens L6
  • ⁇ 7 the dispersion coefficient of the seventh lens L7
  • ⁇ g The dispersion coefficient of the optical filter GF.
  • Table 2 shows the aspheric surface data of each lens in the imaging optical lens 10 of the first embodiment of the present invention.
  • k is the conic coefficient
  • A4, A6, A8, A10, A12, A14, and A16 are the aspheric coefficients.
  • the aspheric surface of each lens surface uses the aspheric surface shown in the above formula (1).
  • the present invention is not limited to the aspheric polynomial form represented by the formula (1).
  • Table 3 and Table 4 show the design data of the inflection point and stagnation point of each lens in the imaging optical lens 10 of the first embodiment of the present invention.
  • P1R1 and P1R2 represent the object side and image side of the first lens L1 respectively
  • P2R1 and P2R2 represent the object side and image side of the second lens L2 respectively
  • P3R1 and P3R2 represent the object side and image side of the third lens L3 respectively.
  • P4R1, P4R2 represent the object side and image side of the fourth lens L4
  • P5R1, P5R2 represent the object side and image side of the fifth lens L5
  • P6R1, P6R2 represent the object side and image side of the sixth lens L6,
  • P7R1 P7R2 represents the object side and image side of the seventh lens L7, respectively.
  • the corresponding data in the “reflection point position” column is the vertical distance from the reflex point set on the surface of each lens to the optical axis of the imaging optical lens 10.
  • the data corresponding to the “stationary point position” column is the vertical distance from the stationary point set on the surface of each lens to the optical axis of the imaging optical lens 10.
  • FIG. 4 shows a schematic diagram of field curvature and distortion of light with a wavelength of 555 nm after passing through the imaging optical lens 10 of the first embodiment.
  • the field curvature S in FIG. 4 is the field curvature in the sagittal direction, and T is the field curvature in the meridian direction. .
  • Table 13 shows the values corresponding to the various values in the first, second, and third embodiments and the parameters specified in the conditional expressions.
  • the first embodiment satisfies various conditional expressions.
  • the entrance pupil diameter of the imaging optical lens 10 is 1.556 mm
  • the full-field image height is 3.25 mm
  • the maximum field angle is 100.92°, making the imaging optical lens 10 wide-angle and ultra-thin. , Its on-axis and off-axis chromatic aberrations are fully corrected, and it has excellent optical characteristics.
  • the second embodiment is basically the same as the first embodiment, and the meaning of the symbols is the same as that of the first embodiment.
  • the structure of the imaging optical lens 20 of the second embodiment is shown in FIG. 5, and only the differences are listed below.
  • the first lens L1 is made of plastic
  • the second lens L2 is made of plastic
  • the third lens L3 is made of glass
  • the fourth lens L4 is made of plastic
  • the fifth lens L5 is made of plastic
  • the sixth lens L6 is made of plastic
  • the seventh lens is made of plastic.
  • the lens L7 is made of plastic.
  • Table 5 and Table 6 show design data of the imaging optical lens 20 according to the second embodiment of the present invention.
  • Table 6 shows the aspheric surface data of each lens in the imaging optical lens 20 according to the second embodiment of the present invention.
  • Table 7 and Table 8 show the design data of the inflection point and stagnation point of each lens in the imaging optical lens 20 according to the second embodiment of the present invention.
  • P2R1 1 0.855 0 P2R2 0 0 0 G3R1 0 0 G3R2 1 0.775 0 P4R1 1 0.165 0 P4R2 1 0.435 0 P5R1 1 0.665 0 P5R2 0 0 0 P6R1 1 0.275 0 P6R2 1 1.435 0 P7R1 2 0.485 1.745 P7R2 2 0.625 2.485
  • FIG. 6 and 7 respectively show schematic diagrams of axial aberration and chromatic aberration of magnification after light having wavelengths of 470 nm, 555 nm, and 650 nm pass through the imaging optical lens 20 of the second embodiment.
  • FIG. 8 shows a schematic diagram of field curvature and distortion of light with a wavelength of 555 nm after passing through the imaging optical lens 20 of the second embodiment.
  • the entrance pupil diameter of the imaging optical lens is 1.036mm
  • the full field of view image height is 3.25mm
  • the maximum field of view is 134.20°, which makes the imaging optical lens 20 wide-angle and ultra-thin.
  • the on-axis and off-axis chromatic aberrations are fully corrected, and it has excellent optical characteristics.
  • the third embodiment is basically the same as the first embodiment, and the meaning of the symbols is the same as that of the first embodiment. Please refer to FIG. 9 for the structure of the imaging optical lens 30 of the third embodiment. Only the differences are listed below.
  • the first lens L1 is made of plastic
  • the second lens L2 is made of plastic
  • the third lens L3 is made of glass
  • the fourth lens L4 is made of plastic
  • the fifth lens L5 is made of plastic
  • the sixth lens L6 is made of plastic
  • the seventh lens is made of plastic.
  • the lens L7 is made of plastic.
  • Table 9 and Table 10 show design data of the imaging optical lens 30 according to the third embodiment of the present invention.
  • Table 10 shows the aspheric surface data of each lens in the imaging optical lens 30 according to the third embodiment of the present invention.
  • Table 11 and Table 12 show the design data of the inflection point and stagnation point of each lens in the imaging optical lens 30 of the third embodiment of the present invention.
  • FIG. 10 and 11 respectively show schematic diagrams of axial aberration and chromatic aberration of magnification after light having wavelengths of 470 nm, 555 nm, and 650 nm pass through the imaging optical lens 30 of the third embodiment.
  • FIG. 12 shows a schematic diagram of field curvature and distortion of light with a wavelength of 555 nm after passing through the imaging optical lens 30 of the third embodiment.
  • the entrance pupil diameter of the imaging optical lens is 1.036mm
  • the full field of view image height is 3.25mm
  • the maximum field of view is 134.20°, making the imaging optical lens 30 wide-angle and ultra-thin.
  • the on-axis and off-axis chromatic aberrations are fully corrected, and it has excellent optical characteristics.
  • Embodiment 1 Embodiment 2
  • Embodiment 3 f 3.423 2.382 2.950 f1 -20.320 -3.714 -6.189 f2 3.746 7.139 6.200 f3 20.919 2.423 3.208 f4 -8.637 -7.794 -3.638
  • Fno is the aperture F number of the imaging optical lens.

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  • Lenses (AREA)

Abstract

L'invention concerne une lentille optique de caméra (10), comprenant dans l'ordre d'un côté objet à un côté image : une première lentille (L1) qui a une réfringence négative, une deuxième lentille (L2) qui a une réfringence positive, une troisième lentille (L3) qui a une réfringence positive, une quatrième lentille (L4) qui a une réfringence négative, une cinquième lentille (L5), une sixième lentille (L6), et une septième lentille (L7), le champ de vision maximal de la lentille optique de caméra (10) étant FOV, la distance focale de la seconde lentille (L2) étant f2, la distance focale de la lentille optique de caméra (10) étant f, l'épaisseur sur l'axe de la troisième lentille (L3) étant d5, l'épaisseur sur l'axe de la septième lentille (L7) étant d13, le coefficient de dispersion de la troisième lentille (L3) étant v3, le coefficient de dispersion de la cinquième lentille (L5) étant v5, et les relations suivantes étant satisfaites : 100,00°≤FOV≤135,00° ; 1,00≤f2/f≤3,00 ; 1,50≤d5/ d13≤3,00 ; et 2,00≤v3-v5≤20,00. La lentille optique de caméra (10) répond aux exigences de conception de grands angles et d'ultra-minceur tout en présentant une bonne performance optique.
PCT/CN2019/128596 2019-12-26 2019-12-26 Lentille optique de caméra Ceased WO2021128141A1 (fr)

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PCT/CN2019/128596 WO2021128141A1 (fr) 2019-12-26 2019-12-26 Lentille optique de caméra

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Citations (6)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
US4871219A (en) * 1987-11-19 1989-10-03 Texas Instruments Incorporated Wide spectral band infrared refractive lens
US6018414A (en) * 1996-03-04 2000-01-25 Raytheon Company Dual band infrared lens assembly using diffractive optics
CN106324797A (zh) * 2015-06-29 2017-01-11 佳能企业股份有限公司 光学镜头
CN107577032A (zh) * 2017-09-19 2018-01-12 舜宇光学(中山)有限公司 低畸变广角镜头
CN108646390A (zh) * 2018-08-01 2018-10-12 舜宇光学(中山)有限公司 近红外大光圈镜头
CN109960004A (zh) * 2017-12-22 2019-07-02 宁波舜宇车载光学技术有限公司 光学镜头

Patent Citations (6)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
US4871219A (en) * 1987-11-19 1989-10-03 Texas Instruments Incorporated Wide spectral band infrared refractive lens
US6018414A (en) * 1996-03-04 2000-01-25 Raytheon Company Dual band infrared lens assembly using diffractive optics
CN106324797A (zh) * 2015-06-29 2017-01-11 佳能企业股份有限公司 光学镜头
CN107577032A (zh) * 2017-09-19 2018-01-12 舜宇光学(中山)有限公司 低畸变广角镜头
CN109960004A (zh) * 2017-12-22 2019-07-02 宁波舜宇车载光学技术有限公司 光学镜头
CN108646390A (zh) * 2018-08-01 2018-10-12 舜宇光学(中山)有限公司 近红外大光圈镜头

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