WO2022041385A1 - 摄像光学镜头 - Google Patents

摄像光学镜头 Download PDF

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Publication number
WO2022041385A1
WO2022041385A1 PCT/CN2020/118572 CN2020118572W WO2022041385A1 WO 2022041385 A1 WO2022041385 A1 WO 2022041385A1 CN 2020118572 W CN2020118572 W CN 2020118572W WO 2022041385 A1 WO2022041385 A1 WO 2022041385A1
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Prior art keywords
lens
imaging optical
optical lens
ttl
curvature
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PCT/CN2020/118572
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English (en)
French (fr)
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陈佳
孙雯
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诚瑞光学(深圳)有限公司
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Publication of WO2022041385A1 publication Critical patent/WO2022041385A1/zh

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    • GPHYSICS
    • G02OPTICS
    • G02BOPTICAL ELEMENTS, SYSTEMS OR APPARATUS
    • G02B9/00Optical objectives characterised both by the number of the components and their arrangements according to their sign, i.e. + or -
    • G02B9/60Optical objectives characterised both by the number of the components and their arrangements according to their sign, i.e. + or - having five components only
    • GPHYSICS
    • G02OPTICS
    • G02BOPTICAL ELEMENTS, SYSTEMS OR APPARATUS
    • G02B13/00Optical objectives specially designed for the purposes specified below
    • G02B13/001Miniaturised objectives for electronic devices, e.g. portable telephones, webcams, PDAs, small digital cameras
    • G02B13/0015Miniaturised objectives for electronic devices, e.g. portable telephones, webcams, PDAs, small digital cameras characterised by the lens design
    • G02B13/002Miniaturised objectives for electronic devices, e.g. portable telephones, webcams, PDAs, small digital cameras characterised by the lens design having at least one aspherical surface
    • G02B13/0045Miniaturised objectives for electronic devices, e.g. portable telephones, webcams, PDAs, small digital cameras characterised by the lens design having at least one aspherical surface having five or more lenses
    • GPHYSICS
    • G02OPTICS
    • G02BOPTICAL ELEMENTS, SYSTEMS OR APPARATUS
    • G02B13/00Optical objectives specially designed for the purposes specified below
    • G02B13/06Panoramic objectives; So-called "sky lenses" including panoramic objectives having reflecting surfaces
    • GPHYSICS
    • G02OPTICS
    • G02BOPTICAL ELEMENTS, SYSTEMS OR APPARATUS
    • G02B13/00Optical objectives specially designed for the purposes specified below
    • G02B13/18Optical objectives specially designed for the purposes specified below with lenses having one or more non-spherical faces, e.g. for reducing geometrical aberration
    • GPHYSICS
    • G02OPTICS
    • G02BOPTICAL ELEMENTS, SYSTEMS OR APPARATUS
    • G02B27/00Optical systems or apparatus not provided for by any of the groups G02B1/00 - G02B26/00, G02B30/00
    • G02B27/0025Optical systems or apparatus not provided for by any of the groups G02B1/00 - G02B26/00, G02B30/00 for optical correction, e.g. distorsion, aberration

Definitions

  • the 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 purpose of the present invention is to provide an imaging optical lens, which not only has good optical performance, but also has the characteristics of large aperture, ultra-thinning, and wide-angle.
  • embodiments of the present invention provide an imaging optical lens, the imaging optical lens includes five lenses in total, and the five lenses are sequentially from the object side to the image side: a lens, a second lens with negative refractive power, a third lens with positive refractive power, a fourth lens with positive refractive power, and a fifth lens with negative refractive power;
  • At least one of the first lens to the fifth lens includes a free-form surface
  • the overall focal length of the imaging optical lens is f
  • the focal length of the third lens is f3
  • the second lens has a focal length on the object side.
  • the central radius of curvature is R3
  • the central radius of curvature of the image side surface of the second lens is R4, and the following relational expressions are satisfied: 2.00 ⁇ f3/f ⁇ 5.50; 2.00 ⁇ R4/R3 ⁇ 23.00.
  • the on-axis thickness of the fourth lens is d7
  • the on-axis distance from the image side of the fourth lens to the object side of the fifth lens is d8, and the following relationship is satisfied: 1.00 ⁇ d7/d8 ⁇ 11.00.
  • the focal length of the first lens is f1
  • the central radius of curvature of the object side of the first lens is R1
  • the central radius of curvature of the image side of the first lens is R2
  • the on-axis thickness of the first lens is is d1
  • the total optical length of the imaging optical lens is TTL, and satisfies the following relationship: 0.46 ⁇ f1/f ⁇ 1.55; -3.88 ⁇ (R1+R2)/(R1-R2) ⁇ -1.02; 0.06 ⁇ d1/ TTL ⁇ 0.22.
  • the focal length of the second lens is f2
  • the on-axis thickness of the second lens is d3
  • the total optical length of the imaging optical lens is TTL, and the following relationship is satisfied: -6.97 ⁇ f2/f ⁇ - 1.24; -5.62 ⁇ (R3+R4)/(R3-R4) ⁇ -0.73; 0.02 ⁇ d3/TTL ⁇ 0.08.
  • the central radius of curvature of the object side of the third lens is R5
  • the central radius of curvature of the image side of the third lens is R6
  • the on-axis thickness of the third lens is d5
  • the optical The total length is TTL and satisfies the following relationship: -3.37 ⁇ (R5+R6)/(R5-R6) ⁇ 0.16; 0.03 ⁇ d5/TTL ⁇ 0.26.
  • the focal length of the fourth lens is f4
  • the central radius of curvature of the object side of the fourth lens is R7
  • the central radius of curvature of the image side of the fourth lens is R8, and the on-axis thickness of the fourth lens is is d7
  • the total optical length of the imaging optical lens is TTL, and satisfies the following relationship: 0.55 ⁇ f4/f ⁇ 6.42; 0.57 ⁇ (R7+R8)/(R7-R8) ⁇ 2.93; 0.06 ⁇ d7/TTL ⁇ 0.19.
  • the focal length of the fifth lens is f5
  • the central radius of curvature of the object side of the fifth lens is R9
  • the central radius of curvature of the image side of the fifth lens is R10
  • the on-axis thickness of the fifth lens is is d9
  • the total optical length of the imaging optical lens is TTL, and satisfies the following relationship: -3.13 ⁇ f5/f ⁇ -0.51; 0.74 ⁇ (R9+R10)/(R9-R10) ⁇ 4.97; 0.05 ⁇ d9/ TTL ⁇ 0.25.
  • the total optical length of the imaging optical lens is TTL
  • the image height of the imaging optical lens is IH
  • the following relational formula is satisfied: TTL/IH ⁇ 1.60.
  • the field of view of the imaging optical lens is FOV, and satisfies the following relationship: FOV ⁇ 77°.
  • the aperture value of the imaging optical lens is FNO, and satisfies the following relationship: FNO ⁇ 2.21.
  • the imaging optical lens according to the present invention has the characteristics of large aperture, ultra-thinning and wide-angle, while having good optical performance, and at the same time, from the first lens to the fifth lens, at least one lens contains Free-form surface helps to correct system distortion and field curvature and improve image quality. It is especially suitable for mobile phone camera lens assemblies and WEB camera lenses composed of high-pixel CCD, CMOS and other camera elements.
  • FIG. 1 is a schematic structural diagram of an imaging optical lens according to a first embodiment of the present invention
  • Fig. 2 is the corresponding situation of the RMS spot diameter of the imaging optical lens shown in Fig. 1 and the real light image height;
  • FIG. 3 is a schematic structural diagram of an imaging optical lens according to a second embodiment of the present invention.
  • Fig. 4 is the corresponding situation of the RMS spot diameter of the imaging optical lens shown in Fig. 3 and the real light image height;
  • FIG. 5 is a schematic structural diagram of an imaging optical lens according to a third embodiment of the present invention.
  • Fig. 6 is the corresponding situation of the RMS spot diameter of the imaging optical lens shown in Fig. 5 and the real light image height;
  • FIG. 7 is a schematic structural diagram of an imaging optical lens according to a fourth embodiment of the present invention.
  • FIG. 8 is the correspondence between the RMS spot diameter of the imaging optical lens shown in FIG. 7 and the real ray image height.
  • FIG. 1 shows an imaging optical lens 10 according to a first embodiment of the present invention, and the imaging optical lens 10 includes five lenses.
  • the imaging optical lens 10 includes, from the object side to the image side, an aperture S1, a first lens L1, a second lens L2, a third lens L3, a fourth lens L4, and a fifth lens L5.
  • Optical elements such as an optical filter GF may be disposed between the fifth lens L5 and the image plane Si.
  • the first lens L1 is made of plastic material
  • the second lens L2 is made of plastic material
  • the third lens L3 is made of plastic material
  • the fourth lens L4 is made of plastic material
  • the fifth lens L5 is made of plastic material.
  • each lens may also be made of other materials.
  • At least one of the first lens L1 to the fifth lens L5 includes a free-form surface, and the free-form surface helps to correct system distortion and field curvature and improve imaging quality.
  • the overall focal length of the imaging optical lens 10 is defined as f
  • the focal length of the third lens L3 is defined as f3, which satisfies the following relationship: 2.00 ⁇ f3/f ⁇ 5.50, which specifies that the focal length of the third lens and the imaging
  • the ratio of the overall focal length of an optical lens to help improve image quality within a range of conditions Preferably, 2.21 ⁇ f3/f ⁇ 5.48 is satisfied.
  • the central radius of curvature of the object side of the second lens L2 is defined as R3, and the central radius of curvature of the image side of the second lens L2 is R4, which satisfies the following relationship: 2.00 ⁇ R4/R3 ⁇ 23.00, which specifies that the second lens has a
  • the shape helps to reduce the degree of light deflection and improve the imaging quality within the range of conditions.
  • the axial thickness of the fourth lens L4 is defined as d7, and the axial distance from the image side of the fourth lens L4 to the object side of the fifth lens is d8, which satisfies the following relationship: 1.00 ⁇ d7/d8 ⁇ 11.00, when d7/d8 meets the conditions, it can help to reduce the total length of the system. Preferably, 1.17 ⁇ d7/d8 ⁇ 10.64 is satisfied.
  • the first lens L1 has a positive refractive power
  • the object side surface is convex at the paraxial position
  • the image side surface is concave at the paraxial position.
  • the focal length of the first lens L1 is defined as f1, and the overall focal length of the imaging optical lens 10 is f, which satisfies the following relationship: 0.46 ⁇ f1/f ⁇ 1.55, which specifies the ratio of the focal length of the first lens L1 to the overall focal length .
  • the first lens has an appropriate positive refractive power, which is conducive to reducing system aberrations, and at the same time, is conducive to the development of ultra-thin and wide-angle lenses.
  • 0.74 ⁇ f1/f ⁇ 1.24 is satisfied.
  • the central radius of curvature of the object side of the first lens L1 is R1, and the central radius of curvature of the image side of the first lens L1 is R2, which satisfy the following relationship: -3.88 ⁇ (R1+R2)/(R1-R2) ⁇ -1.02, the shape of the first lens L1 is reasonably controlled, so that the first lens L1 can effectively correct the spherical aberration of the system.
  • -2.42 ⁇ (R1+R2)/(R1-R2) ⁇ -1.27 is satisfied.
  • the on-axis thickness of the first lens L1 is d1
  • the total optical length of the imaging optical lens 10 is TTL, which satisfies the following relational formula: 0.06 ⁇ d1/TTL ⁇ 0.22, which is conducive to realizing ultra-thinning.
  • 0.09 ⁇ d1/TTL ⁇ 0.17 is satisfied.
  • the second lens L2 has a negative refractive power
  • the object side surface is concave at the paraxial position
  • the image side surface is convex at the paraxial position.
  • the focal length of the second lens L2 is defined as f2, and the overall focal length of the imaging optical lens 10 is f, which satisfies the following relationship: -6.97 ⁇ f2/f ⁇ -1.24, by taking the negative refractive power of the second lens L2 Controlling within a reasonable range is conducive to correcting the aberration of the optical system.
  • -4.36 ⁇ f2/f ⁇ -1.56 is satisfied.
  • the central radius of curvature of the object side surface of the second lens L2 is R3, and the central radius of curvature of the image side surface of the second lens L2 is R4, which satisfy the following relationship: -5.62 ⁇ (R3+R4)/(R3-R4) ⁇ - 0.73, which specifies the shape of the second lens L2.
  • R3+R4 the central radius of curvature of the image side surface of the second lens L2
  • R4 which satisfy the following relationship: -5.62 ⁇ (R3+R4)/(R3-R4) ⁇ - 0.73, which specifies the shape of the second lens L2.
  • it is within the range, as the lens develops to ultra-thin and wide-angle, it is beneficial to correct the problem of axial chromatic aberration.
  • it satisfies -3.51 ⁇ (R3+R4)/( R3-R4) ⁇ -0.91.
  • the on-axis thickness of the second lens L2 is d3, and the total optical length of the imaging optical lens 10 is TTL, which satisfies the following relational formula: 0.02 ⁇ d3/TTL ⁇ 0.08, which is conducive to realizing ultra-thinning. Preferably, 0.04 ⁇ d3/TTL ⁇ 0.06 is satisfied.
  • the third lens L3 has a positive refractive power, the object side surface is convex at the paraxial position, and the image side surface is convex at the paraxial position.
  • the central radius of curvature of the object side of the third lens L3 is defined as R5, and the central radius of curvature of the image side of the third lens L3 is R6, which satisfies the following relationship: -3.37 ⁇ (R5+R6)/(R5-R6) ⁇ 0.16 , specifies the shape of the third lens, within the range specified by the conditional formula, it can ease the degree of deflection of the light passing through the lens, and effectively reduce the aberration.
  • -2.11 ⁇ (R5+R6)/(R5-R6) ⁇ 0.13 is satisfied.
  • the axial thickness of the third lens L3 is d5, and the total optical length of the imaging optical lens 10 is TTL, which satisfies the following relationship: 0.03 ⁇ d5/TTL ⁇ 0.26, which is conducive to realizing ultra-thinning. Preferably, 0.06 ⁇ d5/TTL ⁇ 0.20 is satisfied.
  • the fourth lens L4 has a positive refractive power
  • the object side surface is concave at the paraxial position
  • the image side surface is convex at the paraxial position.
  • the focal length of the fourth lens L4 is defined as f4, and the overall focal length of the imaging optical lens 10 is f, which satisfies the following relationship: 0.55 ⁇ f4/f ⁇ 6.42, which specifies the ratio of the focal length of the fourth lens to the system focal length.
  • Conditional expressions help to improve the performance of the optical system. Preferably, 0.88 ⁇ f4/f ⁇ 5.14 is satisfied.
  • the central radius of curvature of the object side of the fourth lens L4 is R7
  • the central radius of curvature of the image side of the fourth lens L4 is R8, which satisfy the following relationship: 0.57 ⁇ (R7+R8)/(R7-R8) ⁇ 2.93 , which specifies the shape of the fourth lens L4.
  • the shape is within the range, it is beneficial to correct problems such as aberrations of the off-axis picture angle with the development of ultra-thin and wide-angle.
  • 0.91 ⁇ (R7+R8)/(R7-R8) ⁇ 2.35 is satisfied.
  • the axial thickness of the fourth lens L4 is d7, and the optical total length of the imaging optical lens 10 is TTL, which satisfies the following relational formula: 0.06 ⁇ d7/TTL ⁇ 0.19, which is conducive to realizing ultra-thinning. Preferably, 0.09 ⁇ d7/TTL ⁇ 0.16 is satisfied.
  • the fifth lens L5 has a negative refractive power
  • the object side surface is convex at the paraxial position
  • the image side surface is concave at the paraxial position.
  • the focal length of the fifth lens L5 is defined as f5, and the overall focal length of the imaging optical lens 10 is f, which satisfies the following relationship: -3.13 ⁇ f5/f ⁇ -0.51, the limitation of the fifth lens L5 can effectively make
  • the light angle of the camera lens is flat, reducing tolerance sensitivity.
  • -1.96 ⁇ f5/f ⁇ -0.64 is satisfied.
  • the central radius of curvature of the object side of the fifth lens is R9
  • the central radius of curvature of the image side of the fifth lens is R10
  • the following relationship is satisfied: 0.74 ⁇ (R9+R10)/(R9-R10) ⁇ 4.97
  • 1.19 ⁇ (R9+R10)/(R9-R10) ⁇ 3.97 is satisfied.
  • the on-axis thickness of the fifth lens L5 is d9, and the total optical length of the imaging optical lens 10 is TTL, which satisfies the following relationship: 0.05 ⁇ d9/TTL ⁇ 0.25, which is conducive to realizing ultra-thinning.
  • 0.09 ⁇ d9/TTL ⁇ 0.20 is satisfied.
  • the total optical length of the imaging optical lens 10 is TTL
  • the image height of the imaging optical lens 10 is IH, which satisfies the following relation: TTL/IH ⁇ 1.60, thereby realizing ultra-thinning.
  • the field of view of the imaging optical lens is FOV, and satisfies the following relational formula: FOV ⁇ 77°, so as to achieve a wide angle.
  • the aperture value FNO of the imaging optical lens 10 is less than or equal to 2.21, the aperture is large, and the imaging performance is good.
  • the imaging optical lens 10 has good optical performance, and at the same time, the free-form surface can be used to match the designed image area with the actual use area, and the image quality of the effective area can be improved to the greatest extent;
  • the imaging optical lens 10 is especially suitable for mobile phone camera lens assemblies and WEB camera lenses composed of high-pixel CCD, CMOS and other imaging elements.
  • the imaging optical lens 10 of the present invention will be described below by way of examples.
  • the symbols described in each example are as follows.
  • the unit of focal length, on-axis distance, center curvature radius, and on-axis thickness is mm.
  • TTL total optical length (the on-axis distance from the object side of the first lens L1 to the imaging plane), in mm;
  • Aperture value FNO refers to the ratio of the effective focal length of the imaging optical lens to the diameter of the entrance pupil.
  • Table 1 and Table 2 show design data of the imaging optical lens 10 according to the first embodiment of the present invention.
  • the object side surface and the image side surface of the fifth lens L5 are free-form surfaces, and in other embodiments, the free-form surfaces may also exist in multiple lenses at the same time.
  • R the radius of curvature at the center of the optical surface
  • R1 the central radius of curvature of the object side surface of the first lens L1;
  • R2 the central curvature radius of the image side surface of the first lens L1;
  • R3 the central radius of curvature of the object side surface of the second lens L2;
  • R4 the central curvature radius of the image side surface of the second lens L2;
  • R5 the central radius of curvature of the object side surface of the third lens L3;
  • R6 the central curvature radius of the image side surface of the third lens L3;
  • R7 the central curvature radius of the object side surface of the fourth lens L4;
  • R8 the central curvature radius of the image side surface of the fourth lens L4;
  • R9 the central curvature radius of the object side surface of the fifth lens L5;
  • R10 the central curvature radius of the image side surface of the fifth lens L5;
  • R11 the central curvature radius of the object side of the optical filter GF
  • R12 the central curvature radius of the image side of the optical filter GF
  • d the on-axis thickness of the lens, the on-axis distance between the lenses
  • d0 the on-axis distance from the aperture S1 to the object side surface of the first lens L1;
  • d2 the on-axis distance from the image side of the first lens L1 to the object side of the second lens L2;
  • d4 the on-axis distance from the image side of the second lens L2 to the object side of the third lens L3;
  • d6 the on-axis distance from the image side of the third lens L3 to the object side of the fourth lens L4;
  • d10 the axial distance from the image side of the fifth lens L5 to the image side of the optical filter GF to the image plane;
  • d11 On-axis thickness of optical filter GF
  • d12 the axial distance from the image side of the optical filter GF to the image plane
  • nd the refractive index of the 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;
  • ndg the refractive index of the d-line of the optical filter GF
  • vg Abbe number of optical filter GF.
  • Table 2 shows aspherical surface data of each lens in the imaging optical lens 10 according to the first embodiment of the present invention.
  • k is the conic coefficient
  • A4, A6, A8, A10, A12, A14, A16, A18, A20 are the aspheric coefficients
  • c is the curvature at the center of the optical surface
  • r is the vertical distance between the point on the aspheric curve and the optical axis
  • z is the depth of the aspheric surface (the vertical distance between a point on the aspheric surface with a distance r from the optical axis and a tangent plane tangent to the vertex on the optical axis of the aspheric surface).
  • the aspherical surface shown in the above formula (1) is used as the aspherical surface of each lens surface.
  • the present invention is not limited to the aspheric polynomial form represented by the formula (1).
  • Table 3 shows free-form surface data in the imaging optical lens 10 according to the first embodiment of the present invention.
  • k is the conic coefficient
  • Bi is the aspheric coefficient
  • c is the optical surface
  • r is the vertical distance between the point on the free-form surface and the optical axis
  • x is the x-direction component of r
  • y is the y-direction component of r
  • z is the depth of the aspheric surface (the point on the aspheric surface with a distance from the optical axis r , and the vertical distance between the tangent plane tangent to the vertex on the aspheric optical axis).
  • N 63
  • N can also take other values.
  • each free-form surface uses the Extended Polynomial surface type shown in the above formula (2).
  • the present invention is not limited to the free-form surface polynomial form represented by the formula (2).
  • FIG. 2 shows the correspondence between the RMS spot diameter and the true light image height of the imaging optical lens 10 of the first embodiment. It can be seen from FIG. 2 that the imaging optical lens 10 of the first embodiment can achieve good imaging quality.
  • Table 13 shows the values corresponding to the various numerical values in each of Examples 1, 2, 3, and 4 and the parameters specified in the conditional expressions.
  • the first embodiment satisfies each conditional expression.
  • the entrance pupil diameter ENPD of the imaging optical lens 10 is 1.770mm
  • the full field of view image height (diagonal direction) IH is 6.940mm
  • the image height in the x direction is 5.200mm
  • the image height in the y direction is 4.600mm
  • the imaging effect is the best in this rectangular range.
  • the FOV in the diagonal direction is 87.13°
  • the field angle in the x direction is 70.99°
  • the field angle in the y direction is 64.45°.
  • the lens 10 meets the design requirements of wide-angle, ultra-thin, and large aperture, 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, the meanings of symbols are the same as those of the first embodiment, and only the differences are listed below.
  • Table 4 and Table 5 show design data of the imaging optical lens 20 according to the second embodiment of the present invention.
  • the object side surface and the image side surface of the second lens L2 are free-form surfaces, and in other embodiments, the free-form surfaces may also exist in multiple lenses at the same time.
  • Table 5 shows aspherical surface data of each lens in the imaging optical lens 20 according to the second embodiment of the present invention.
  • Table 6 shows free-form surface data in the imaging optical lens 20 according to the second embodiment of the present invention.
  • FIG. 4 shows the correspondence between the RMS spot diameter and the true light image height of the imaging optical lens 20 of the second embodiment. It can be seen from FIG. 4 that the imaging optical lens 20 of the second embodiment can achieve good imaging quality.
  • the second embodiment satisfies each conditional expression.
  • the entrance pupil diameter ENPD of the imaging optical lens 20 is 1.783mm
  • the full field of view image height (diagonal direction) IH is 6.940mm
  • the image height in the x direction is 5.200mm
  • the image height in the y direction is 4.600mm
  • the imaging effect is the best in this rectangular range.
  • the FOV in the diagonal direction is 86.33°
  • the field angle in the x direction is 70.39°
  • the field angle in the y direction is 63.97°.
  • the lens 20 meets the design requirements of wide-angle, ultra-thin, and large aperture, its 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, the meanings of symbols are the same as those of the first embodiment, and only the differences are listed below.
  • the image side surface of the third lens L3 is concave at the paraxial position.
  • Tables 7 and 8 show design data of the imaging optical lens 30 according to the third embodiment of the present invention.
  • Table 8 shows aspherical surface data of each lens in the imaging optical lens 30 according to the third embodiment of the present invention.
  • Table 9 shows free-form surface data in the imaging optical lens 30 according to the third embodiment of the present invention.
  • FIG. 6 shows the correspondence between the RMS spot diameter of the imaging optical lens 30 of the third embodiment and the true light image height. It can be seen from FIG. 6 that the imaging optical lens 30 of the third embodiment can achieve good imaging quality.
  • the entrance pupil diameter ENPD of the imaging optical lens 30 is 1.682 mm
  • the full field of view image height (diagonal direction) IH is 6.000 mm
  • the image height in the x direction is 4.800 mm
  • the image height in the y direction is 3.600mm
  • the imaging effect is the best in this rectangular range.
  • the FOV in the diagonal direction is 78.00°
  • the field angle in the x direction is 65.69°
  • the field angle in the y direction is 51.24°.
  • the lens 30 meets the design requirements of wide-angle, ultra-thin, and large aperture, its on-axis and off-axis chromatic aberrations are fully corrected, and it has excellent optical characteristics.
  • the fourth embodiment is basically the same as the first embodiment, the meanings of symbols are the same as those of the first embodiment, and only the differences are listed below.
  • the image side surface of the third lens L3 is concave at the paraxial position.
  • Table 10 and Table 11 show design data of the imaging optical lens 40 according to the fourth embodiment of the present invention. Among them, only the object side surface and the image side surface of the first lens L1 are free-form surfaces, and in other embodiments, the free-form surfaces may exist in multiple lenses at the same time.
  • Table 11 shows aspherical surface data of each lens in the imaging optical lens 40 according to the fourth embodiment of the present invention.
  • Table 12 shows free-form surface data in the imaging optical lens 40 according to the fourth embodiment of the present invention.
  • Fig. 8 shows the correspondence between the RMS spot diameter and the true ray image height of the imaging optical lens 40 of the fourth embodiment. It can be seen from Fig. 8 that the imaging optical lens 40 of the fourth embodiment can achieve good imaging quality.
  • the entrance pupil diameter ENPD of the imaging optical lens 40 is 1.695mm
  • the full field of view image height (diagonal direction) IH is 6.000mm
  • the image height in the x direction is 4.800mm
  • the image height in the y direction is 3.600mm
  • the imaging effect is the best in this rectangular range.
  • the FOV in the diagonal direction is 77.50°
  • the field angle in the x direction is 64.95°
  • the field angle in the y direction is 50.70°.
  • the lens 40 meets the design requirements of wide-angle, ultra-thin, and large aperture, its on-axis and off-axis chromatic aberrations are fully corrected, and it has excellent optical characteristics.

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Abstract

一种摄像光学镜头(10),共包含五片透镜,五片透镜由物侧至像侧依次为:第一透镜(L1),第二透镜(L2),第三透镜(L3),第四透镜(L4),以及第五透镜(L5);其中,第一透镜(L1)至第五透镜(L5)中的至少一个含自由曲面,摄像光学镜头(10)整体的焦距为f,第三透镜(L3)的焦距为f3,第二透镜(L2)物侧面的中心曲率半径为R3,第二透镜(L2)像侧面的中心曲率半径为R4,且满足下列关系式:2.00≤f3/f≤5.50;2.00≤R4/R3≤23.00。这种摄像光学镜头(10)具有良好光学性能的同时,满足超薄化、广角化、大光圈的设计要求。

Description

摄像光学镜头 技术领域
本发明涉及光学镜头领域,特别涉及一种适用于智能手机、数码相机等手提终端设备,以及监视器、PC镜头等摄像装置的摄像光学镜头。
背景技术
随着成像镜头的发展,人们对镜头的成像要求越来越高,镜头的“夜景拍照”和“背景虚化”也成为衡量镜头成像标准的重要指标。目前多采用旋转对称的非球面,这类非球面只在子午平面内具有充分的自由度,并不能很好的对轴外像差进行校正。且现有结构光焦度分配、透镜间隔和透镜形状设置不充分,造成镜头超薄化和广角化不充分。自由曲面是一种非旋转对称的表面类型,能够更好地平衡像差,提高成像质量,而且自由曲面的加工也逐渐成熟。随着对镜头成像要求的提升,在设计镜头时加入自由曲面显得十分重要,尤其是在广角和超广角镜头的设计中效果更为明显。
发明内容
针对上述问题,本发明的目的在于提供一种摄像光学镜头,其具有良好光学性能的同时,具有大光圈、超薄化、广角化的特点。
为解决上述技术问题,本发明的实施方式提供了一种摄像光学镜头,所述摄像光学镜头共包含五片透镜,五片所述透镜由物侧至像侧依次为:具有正屈折力的第一透镜,具有负屈折力的第二透镜,具有正屈折力的第三透镜,具有正屈折力的第四透镜,以及具有负屈折力的第五透镜;
其中,所述第一透镜至所述第五透镜中的至少一个含自由曲面,所述摄像光学镜头整体的焦距为f,所述第三透镜的焦距为f3,所述第二透镜物侧面的中心曲率半径为R3,所述第二透镜像侧面的中心曲率半径为R4,且满足下列关系式:2.00≤f3/f≤5.50;2.00≤R4/R3≤23.00。
优选地,所述第四透镜的轴上厚度为d7,所述第四透镜的像侧面到所述第五透镜的物侧面的轴上距离为d8,且满足下列关系式:1.00≤d7/d8≤11.00。
优选地,所述第一透镜的焦距为f1,所述第一透镜物侧面的中心曲率半径为R1,所述第一透镜像侧面的中心曲率半径为R2,所述第一透镜的轴上厚度为d1,所述摄像光学镜头的光学总长为TTL,且满足下列关系式:0.46≤f1/f≤1.55;-3.88≤(R1+R2)/(R1-R2)≤-1.02;0.06≤d1/TTL≤0.22。
优选地,所述第二透镜的焦距为f2,所述第二透镜的轴上厚度为d3,所述摄像光学镜头的光学总长为TTL,且满足下列关系式:-6.97≤f2/f≤-1.24;-5.62≤(R3+R4)/(R3-R4)≤-0.73;0.02≤d3/TTL≤0.08。
优选地,所述第三透镜物侧面的中心曲率半径为R5,所述第三透镜像侧面的中心曲率半径为R6,所述第三透镜的轴上厚度为d5,所述摄像光学镜头的光学总长为TTL,且满足下列关系式:-3.37≤(R5+R6)/(R5-R6)≤0.16;0.03≤d5/TTL≤0.26。
优选地,所述第四透镜的焦距为f4,所述第四透镜物侧面的中心曲率半径为R7,所述第四透镜像侧面的中心曲率半径为R8,所述第四透镜的轴上厚度为d7,所述摄像光学镜头的光学总长为TTL,且满足下列关系式:0.55≤f4/f≤6.42;0.57≤(R7+R8)/(R7-R8)≤2.93;0.06≤d7/TTL≤0.19。
优选地,所述第五透镜的焦距为f5,所述第五透镜物侧面的中心 曲率半径为R9,所述第五透镜像侧面的中心曲率半径为R10,所述第五透镜的轴上厚度为d9,所述摄像光学镜头的光学总长为TTL,且满足下列关系式:-3.13≤f5/f≤-0.51;0.74≤(R9+R10)/(R9-R10)≤4.97;0.05≤d9/TTL≤0.25。
优选地,所述摄像光学镜头的光学总长为TTL,所述摄像光学镜头的像高为IH,且满足下列关系式:TTL/IH≤1.60。
优选地,所述摄像光学镜头的视场角为FOV,且满足下列关系式:FOV≥77°。
优选地,所述摄像光学镜头的光圈值为FNO,且满足下列关系式:FNO≤2.21。
本发明的有益效果在于:根据本发明的摄像光学镜头具有良好光学性能的同时,具有大光圈、超薄化、广角化的特点,同时,从第一透镜到第五透镜,至少有一个透镜含有自由曲面,有助于校正系统畸变、场曲,提高成像质量,尤其适用于由高像素用的CCD、CMOS等摄像元件构成的手机摄像镜头组件和WEB摄像镜头。
附图说明
为了更清楚地说明本发明实施方式中的技术方案,下面将对实施方式描述中所需要使用的附图作简单地介绍,显而易见地,下面描述中的附图仅仅是本发明的一些实施方式,对于本领域普通技术人员来讲,在不付出创造性劳动的前提下,还可以根据这些附图获得其它的附图,其中:
图1是本发明第一实施方式的摄像光学镜头的结构示意图;
图2是图1所示摄像光学镜头的RMS光斑直径与真实光线像高的对应情况;
图3是本发明第二实施方式的摄像光学镜头的结构示意图;
图4是图3所示摄像光学镜头的RMS光斑直径与真实光线像高的对应情况;
图5是本发明第三实施方式的摄像光学镜头的结构示意图;
图6是图5所示摄像光学镜头的RMS光斑直径与真实光线像高的对应情况;
图7是本发明第四实施方式的摄像光学镜头的结构示意图;
图8是图7所示摄像光学镜头的RMS光斑直径与真实光线像高的对应情况。
具体实施方式
为使本发明的目的、技术方案和优点更加清楚,下面将结合附图对本发明的各实施方式进行详细的阐述。然而,本领域的普通技术人员可以理解,在本发明各实施方式中,为了使读者更好地理解本发明而提出了许多技术细节。但是,即使没有这些技术细节和基于以下各实施方式的种种变化和修改,也可以实现本发明所要求保护的技术方案。
(第一实施方式)
参考附图,本发明提供了一种摄像光学镜头10。图1所示为本发明第一实施方式的摄像光学镜头10,该摄像光学镜头10包括五个透镜。具体的,所述摄像光学镜头10,由物侧至像侧依序包括:光圈S1、第一透镜L1、第二透镜L2、第三透镜L3、第四透镜L4、第五透镜L5。第五透镜L5和像面Si之间可设置有光学过滤片(filter)GF等光学元件。
在本实施方式中,第一透镜L1为塑料材质,第二透镜L2为塑料 材质,第三透镜L3为塑料材质,第四透镜L4为塑料材质,第五透镜L5为塑料材质。在其他实施例中,各透镜也可以是其他材质。
本实施方式中,所述第一透镜L1至所述第五透镜L5中的至少一个含自由曲面,自由曲面有助于校正系统畸变、场曲,提高成像质量。
本实施方式中,定义所述摄像光学镜头10整体的焦距为f,所述第三透镜L3的焦距为f3,满足下列关系式:2.00≤f3/f≤5.50,规定了第三透镜焦距与摄像光学镜头整体的焦距的比值,在条件范围内有助于提高成像质量。优选地,满足2.21≤f3/f≤5.48。
定义所述第二透镜L2物侧面的中心曲率半径为R3,所述第二透镜L2像侧面的中心曲率半径为R4,满足下列关系式:2.00≤R4/R3≤23.00,规定了第二透镜的形状,在条件范围内有助于降低光线偏折程度,提升成像品质。
定义所述第四透镜L4的轴上厚度为d7,所述第四透镜L4的像侧面到所述第五透镜的物侧面的轴上距离为d8,满足下列关系式:1.00≤d7/d8≤11.00,当d7/d8满足条件时,可有助于降低系统总长。优选地,满足1.17≤d7/d8≤10.64。
本实施方式中,所述第一透镜L1具有正屈折力,其物侧面于近轴处为凸面,像侧面于近轴处为凹面。
定义所述第一透镜L1的焦距为f1,所述摄像光学镜头10整体的焦距为f,满足下列关系式:0.46≤f1/f≤1.55,规定了第一透镜L1的焦距与整体焦距的比值。在规定的范围内时,第一透镜具有适当的正屈折力,有利于减小系统像差,同时有利于镜头向超薄化、广角化发展。优选地,满足0.74≤f1/f≤1.24。
所述第一透镜L1物侧面的中心曲率半径为R1,所述第一透镜L1像侧面的中心曲率半径为R2,满足下列关系式:-3.88≤ (R1+R2)/(R1-R2)≤-1.02,合理控制第一透镜L1的形状,使得第一透镜L1能够有效地校正系统球差。优选地,满足-2.42≤(R1+R2)/(R1-R2)≤-1.27。
所述第一透镜L1的轴上厚度为d1,所述摄像光学镜头10的光学总长为TTL,满足下列关系式:0.06≤d1/TTL≤0.22,有利于实现超薄化。优选地,满足0.09≤d1/TTL≤0.17。
本实施方式中,所述第二透镜L2具有负屈折力,其物侧面于近轴处为凹面,像侧面于近轴处为凸面。
定义所述第二透镜L2的焦距为f2,所述摄像光学镜头10整体的焦距为f,满足下列关系式:-6.97≤f2/f≤-1.24,通过将第二透镜L2的负光焦度控制在合理范围,有利于矫正光学系统的像差。优选地,满足-4.36≤f2/f≤-1.56。
所述第二透镜L2物侧面的中心曲率半径为R3,所述第二透镜L2像侧面的中心曲率半径为R4,满足下列关系式-5.62≤(R3+R4)/(R3-R4)≤-0.73,规定了第二透镜L2的形状,在范围内时,随着镜头向超薄广角化发展,有利于补正轴上色像差问题,优选地,满足-3.51≤(R3+R4)/(R3-R4)≤-0.91。
所述第二透镜L2的轴上厚度为d3,所述摄像光学镜头10的光学总长为TTL,满足下列关系式:0.02≤d3/TTL≤0.08,有利于实现超薄化。优选地,满足0.04≤d3/TTL≤0.06。
本实施方式中,所述第三透镜L3具有正屈折力,其物侧面于近轴处为凸面,像侧面于近轴处为凸面。
定义所述第三透镜L3物侧面的中心曲率半径为R5,第三透镜L3像侧面的中心曲率半径为R6,满足下列关系式:-3.37≤(R5+R6)/(R5-R6)≤0.16,规定了第三透镜的形状,在条件式规定范围 内,可以缓和光线经过镜片的偏折程度,有效减小像差。优选地,满足-2.11≤(R5+R6)/(R5-R6)≤0.13。
所述第三透镜L3的轴上厚度为d5,所述摄像光学镜头10的光学总长为TTL,满足下列关系式:0.03≤d5/TTL≤0.26,有利于实现超薄化。优选地,满足0.06≤d5/TTL≤0.20。
本实施方式中,所述第四透镜L4具有正屈折力,其物侧面于近轴处为凹面,像侧面于近轴处为凸面。
定义所述第四透镜L4的焦距为f4,所述摄像光学镜头10整体的焦距为f,满足下列关系式:0.55≤f4/f≤6.42,规定了第四透镜焦距与系统焦距的比值,在条件式范围内有助于提高光学系统性能。优选地,满足0.88≤f4/f≤5.14。
所述第四透镜L4物侧面的中心曲率半径为R7,所述第四透镜L4像侧面的中心曲率半径为R8,满足下列关系式:0.57≤(R7+R8)/(R7-R8)≤2.93,规定了第四透镜L4的形状,在范围内时,随着超薄广角化的发展,有利于补正轴外画角的像差等问题。优选地,满足0.91≤(R7+R8)/(R7-R8)≤2.35。
所述第四透镜L4的轴上厚度为d7,所述摄像光学镜头10的光学总长为TTL,满足下列关系式:0.06≤d7/TTL≤0.19,有利于实现超薄化。优选地,满足0.09≤d7/TTL≤0.16。
本实施方式中,所述第五透镜L5具有负屈折力,其物侧面于近轴处为凸面,像侧面于近轴处为凹面。
定义所述第五透镜L5的焦距为f5,所述摄像光学镜头10整体的焦距为f,满足下列关系式:-3.13≤f5/f≤-0.51,对第五透镜L5的限定可有效的使得摄像镜头的光线角度平缓,降低公差敏感度。优选地,满足-1.96≤f5/f≤-0.64。
所述第五透镜物侧面的中心曲率半径为R9,以及所述第五透镜像侧面的中心曲率半径为R10,且满足下列关系式:0.74≤(R9+R10)/(R9-R10)≤4.97,规定了第五透镜L5的形状,在范围内时,随着超薄广角化的发展,有利于补正轴外画角的像差等问题。优选地,满足1.19≤(R9+R10)/(R9-R10)≤3.97。
所述第五透镜L5的轴上厚度为d9,所述摄像光学镜头10的光学总长为TTL,满足下列关系式:0.05≤d9/TTL≤0.25,有利于实现超薄化。优选地,满足0.09≤d9/TTL≤0.20。
本实施方式中,所述摄像光学镜头10的光学总长为TTL,所述摄像光学镜头10的像高为IH,满足下列关系式:TTL/IH≤1.60,从而实现超薄化。
本实施方式中,所述摄像光学镜头的视场角为FOV,且满足下列关系式:FOV≥77°,从而实现广角化。
本实施方式中,摄像光学镜头10的光圈值FNO小于或等于2.21,大光圈,成像性能好。
当满足上述关系时,使得摄像光学镜头10具有良好光学性能的同时,采用自由曲面,可实现设计像面区域与实际使用区域匹配,最大程度提升有效区域的像质;根据该摄像光学镜头10的特性,该摄像光学镜头10尤其适用于由高像素用的CCD、CMOS等摄像元件构成的手机摄像镜头组件和WEB摄像镜头。
下面将用实例进行说明本发明的摄像光学镜头10。各实例中所记载的符号如下所示。焦距、轴上距离、中心曲率半径、轴上厚度的单位为mm。
TTL:光学总长(第一透镜L1的物侧面到成像面的轴上距离),单位为mm;
光圈值FNO:是指摄像光学镜头的有效焦距和入瞳直径的比值。
表1、表2示出本发明第一实施方式的摄像光学镜头10的设计数据。其中,仅第五透镜L5的物侧面和像侧面为自由曲面,在其他实施方式中,自由曲面也可同时存在于多片透镜中。
【表1】
Figure PCTCN2020118572-appb-000001
其中,各符号的含义如下。
S1:光圈;
R:光学面中心处的曲率半径;
R1:第一透镜L1的物侧面的中心曲率半径;
R2:第一透镜L1的像侧面的中心曲率半径;
R3:第二透镜L2的物侧面的中心曲率半径;
R4:第二透镜L2的像侧面的中心曲率半径;
R5:第三透镜L3的物侧面的中心曲率半径;
R6:第三透镜L3的像侧面的中心曲率半径;
R7:第四透镜L4的物侧面的中心曲率半径;
R8:第四透镜L4的像侧面的中心曲率半径;
R9:第五透镜L5的物侧面的中心曲率半径;
R10:第五透镜L5的像侧面的中心曲率半径;
R11:光学过滤片GF的物侧面的中心曲率半径;
R12:光学过滤片GF的像侧面的中心曲率半径;
d:透镜的轴上厚度、透镜之间的轴上距离;
d0:光圈S1到第一透镜L1的物侧面的轴上距离;
d1:第一透镜L1的轴上厚度;
d2:第一透镜L1的像侧面到第二透镜L2的物侧面的轴上距离;
d3:第二透镜L2的轴上厚度;
d4:第二透镜L2的像侧面到第三透镜L3的物侧面的轴上距离;
d5:第三透镜L3的轴上厚度;
d6:第三透镜L3的像侧面到第四透镜L4的物侧面的轴上距离;
d7:第四透镜L4的轴上厚度;
d8:第四透镜L4的像侧面到第五透镜L5的物侧面的轴上距离;
d9:第五透镜L5的轴上厚度;
d10:第五透镜L5的像侧面到光学过滤片GF的像侧面到像面的轴上距离;
d11:光学过滤片GF的轴上厚度;
d12:光学过滤片GF的像侧面到像面的轴上距离;
nd:d线的折射率;
nd1:第一透镜L1的d线的折射率;
nd2:第二透镜L2的d线的折射率;
nd3:第三透镜L3的d线的折射率;
nd4:第四透镜L4的d线的折射率;
nd5:第五透镜L5的d线的折射率;
ndg:光学过滤片GF的d线的折射率;
vd:阿贝数;
v1:第一透镜L1的阿贝数;
v2:第二透镜L2的阿贝数;
v3:第三透镜L3的阿贝数;
v4:第四透镜L4的阿贝数;
v5:第五透镜L5的阿贝数;
vg:光学过滤片GF的阿贝数。
表2示出本发明第一实施方式的摄像光学镜头10中各透镜的非球面数据。
【表2】
Figure PCTCN2020118572-appb-000002
Figure PCTCN2020118572-appb-000003
z=(cr 2)/{1+[1-(k+1)(c 2r 2)] 1/2}+A4r 4+A6r 6+A8r 8+A10r 10+A12r 12+A14r 14+A16r 16+A18r 18+A20r 20       (1)
其中,k是圆锥系数,A4、A6、A8、A10、A12、A14、A16、A18、A20是非球面系数,c是光学面中心处的曲率,r是非球面曲线上的点与光轴的垂直距离,z是非球面深度(非球面上距离光轴为r的点,与相切于非球面光轴上顶点的切面两者间的垂直距离)。
为方便起见,各个透镜面的非球面使用上述公式(1)中所示的非球面。但是,本发明不限于该公式(1)表示的非球面多项式形式。
表3示出本发明第一实施方式的摄像光学镜头10中的自由曲面数据。
【表3】
Figure PCTCN2020118572-appb-000004
Figure PCTCN2020118572-appb-000005
Figure PCTCN2020118572-appb-000006
其中,k是圆锥系数,Bi是非球面系数,Ei(x,y)=x my n,式中m、n的取值分别对应表3中列出的x my n项,c是光学面中心处的曲率,r是自由曲面上的点与光轴的垂直距离,x是r的x方向分量,y是r的y方向分量,z是非球面深度(非球面上距离光轴为r的点,与相切于非球面光轴上顶点的切面两者间的垂直距离)。,在本实施方式中,N=63,在其他实施方式中,N也可取其他数值。
为方便起见,各个自由曲面使用上述公式(2)中所示的扩展多项式(Extended Polynomial)面型。但是,本发明不限于该公式(2)表示的自由曲面多项式形式。
图2示出了第一实施例的摄像光学镜头10的RMS光斑直径与真实光线像高的对应情况,根据图2可知,第一实施方式的摄像光学镜头10能够实现良好的成像品质。
后出现的表13示出各实例1、2、3、4中各种数值与条件式中已规定的参数所对应的值。
如表13所示,第一实施方式满足各条件式。
在本实施方式中,所述摄像光学镜头10的入瞳直径ENPD为1.770mm,全视场像高(对角线方向)IH为6.940mm,x方向像高为 5.200mm,y方向像高为4.600mm,在此矩形范围内成像效果最佳,对角线方向的视场角FOV为87.13°,x方向的视场角为70.99°,y方向的视场角为64.45°,所述摄像光学镜头10满足广角化、超薄化、大光圈的设计要求,其轴上、轴外色像差被充分补正,且具有优秀的光学特征。
(第二实施方式)
第二实施方式与第一实施方式基本相同,符号含义与第一实施方式相同,以下只列出不同点。
表4、表5示出本发明第二实施方式的摄像光学镜头20的设计数据。其中,仅第二透镜L2的物侧面和像侧面为自由曲面,在其他实施方式中,自由曲面也可同时存在于多片透镜中。
【表4】
Figure PCTCN2020118572-appb-000007
表5示出本发明第二实施方式的摄像光学镜头20中各透镜的非球面数据。
【表5】
Figure PCTCN2020118572-appb-000008
表6示出本发明第二实施方式的摄像光学镜头20中的自由曲面数据。
【表6】
Figure PCTCN2020118572-appb-000009
Figure PCTCN2020118572-appb-000010
图4示出了第二实施例的摄像光学镜头20的RMS光斑直径与真实光线像高的对应情况,根据图4可知,第二实施方式的摄像光学镜头20能够实现良好的成像品质。
如表13所示,第二实施方式满足各条件式。
在本实施方式中,所述摄像光学镜头20的入瞳直径ENPD为1.783mm,全视场像高(对角线方向)IH为6.940mm,x方向像高为5.200mm,y方向像高为4.600mm,在此矩形范围内成像效果最佳,对角线方向的视场角FOV为86.33°,x方向的视场角为70.39°,y方向的视场角为63.97°,所述摄像光学镜头20满足广角化、超薄化、大光圈的设计要求,其轴上、轴外色像差被充分补正,且具有优秀的光学特征。
(第三实施方式)
第三实施方式与第一实施方式基本相同,符号含义与第一实施方式相同,以下只列出不同点。
在本实施方式中,第三透镜L3的像侧面于近轴处为凹面。
表7、表8示出本发明第三实施方式的摄像光学镜头30的设计数据。
【表7】
Figure PCTCN2020118572-appb-000011
Figure PCTCN2020118572-appb-000012
表8示出本发明第三实施方式的摄像光学镜头30中各透镜的非球面数据。
【表8】
Figure PCTCN2020118572-appb-000013
表9示出本发明第三实施方式的摄像光学镜头30中的自由曲面数据。
【表9】
Figure PCTCN2020118572-appb-000014
Figure PCTCN2020118572-appb-000015
图6示出了第三实施例的摄像光学镜头30的RMS光斑直径与真实光线像高的对应情况,根据图6可知,第三实施方式的摄像光学镜头30能够实现良好的成像品质。
以下表13按照上述条件式列出了本实施方式中对应各条件式的数值。显然,本实施方式的摄像光学系统满足上述的条件式。
在本实施方式中,所述摄像光学镜头30的入瞳直径ENPD为1.682mm,全视场像高(对角线方向)IH为6.000mm,x方向像高为4.800mm,y方向像高为3.600mm,在此矩形范围内成像效果最佳,对角线方向的视场角FOV为78.00°,x方向的视场角为65.69°,y方向的视场角为51.24°,所述摄像光学镜头30满足广角化、超薄化、大光圈的设计要求,其轴上、轴外色像差被充分补正,且具有优秀的光学特征。
(第四实施方式)
第四实施方式与第一实施方式基本相同,符号含义与第一实施方式相同,以下只列出不同点。
在本实施方式中,第三透镜L3的像侧面于近轴处为凹面。
表10、表11示出本发明第四实施方式的摄像光学镜头40的设计数据。其中,仅第一透镜L1的物侧面和像侧面为自由曲面,在其他实施方式中,自由曲面也可同时存在于多片透镜中。
【表10】
Figure PCTCN2020118572-appb-000016
表11示出本发明第四实施方式的摄像光学镜头40中各透镜的非球面数据。
【表11】
Figure PCTCN2020118572-appb-000017
Figure PCTCN2020118572-appb-000018
表12示出本发明第四实施方式的摄像光学镜头40中的自由曲面数据。
【表12】
Figure PCTCN2020118572-appb-000019
图8示出了第四实施例的摄像光学镜头40的RMS光斑直径与真 实光线像高的对应情况,根据图8可知,第四实施方式的摄像光学镜头40能够实现良好的成像品质。
以下表13按照上述条件式列出了本实施方式中对应各条件式的数值。显然,本实施方式的摄像光学系统满足上述的条件式。
在本实施方式中,所述摄像光学镜头40的入瞳直径ENPD为1.695mm,全视场像高(对角线方向)IH为6.000mm,x方向像高为4.800mm,y方向像高为3.600mm,在此矩形范围内成像效果最佳,对角线方向的视场角FOV为77.50°,x方向的视场角为64.95°,y方向的视场角为50.70°,所述摄像光学镜头40满足广角化、超薄化、大光圈的设计要求,其轴上、轴外色像差被充分补正,且具有优秀的光学特征。
【表13】
Figure PCTCN2020118572-appb-000020
本领域的普通技术人员可以理解,上述各实施方式是实现本发明的具体实施方式,而在实际应用中,可以在形式上和细节上对其作各种改变,而不偏离本发明的精神和范围。

Claims (10)

  1. 一种摄像光学镜头,其特征在于,所述摄像光学镜头共包含五片透镜,五片所述透镜由物侧至像侧依次为:具有正屈折力的第一透镜,具有负屈折力的第二透镜,具有正屈折力的第三透镜,具有正屈折力的第四透镜,以及具有负屈折力的第五透镜;
    所述第一透镜至所述第五透镜中的至少一个含自由曲面,所述摄像光学镜头整体的焦距为f,所述第三透镜的焦距为f3,所述第二透镜物侧面的中心曲率半径为R3,所述第二透镜像侧面的中心曲率半径为R4,且满足下列关系式:
    2.00≤f3/f≤5.50;
    2.00≤R4/R3≤23.00。
  2. 根据权利要求1所述的摄像光学镜头,其特征在于,所述第四透镜的轴上厚度为d7,所述第四透镜的像侧面到所述第五透镜的物侧面的轴上距离为d8,且满足下列关系式:
    1.00≤d7/d8≤11.00。
  3. 根据权利要求1所述的摄像光学镜头,其特征在于,所述第一透镜的焦距为f1,所述第一透镜物侧面的中心曲率半径为R1,所述第一透镜像侧面的中心曲率半径为R2,所述第一透镜的轴上厚度为d1,所述摄像光学镜头的光学总长为TTL,且满足下列关系式:
    0.46≤f1/f≤1.55;
    -3.88≤(R1+R2)/(R1-R2)≤-1.02;
    0.06≤d1/TTL≤0.22。
  4. 根据权利要求1所述的摄像光学镜头,其特征在于,所述第二透镜的焦距为f2,所述第二透镜的轴上厚度为d3,所述摄像光学镜头的光学总 长为TTL,且满足下列关系式:
    -6.97≤f2/f≤-1.24;
    -5.62≤(R3+R4)/(R3-R4)≤-0.73;
    0.02≤d3/TTL≤0.08。
  5. 根据权利要求1所述的摄像光学镜头,其特征在于,所述第三透镜物侧面的中心曲率半径为R5,所述第三透镜像侧面的中心曲率半径为R6,所述第三透镜的轴上厚度为d5,所述摄像光学镜头的光学总长为TTL,且满足下列关系式:
    -3.37≤(R5+R6)/(R5-R6)≤0.16;
    0.03≤d5/TTL≤0.26。
  6. 根据权利要求1所述的摄像光学镜头,其特征在于,所述第四透镜的焦距为f4,所述第四透镜物侧面的中心曲率半径为R7,所述第四透镜像侧面的中心曲率半径为R8,所述第四透镜的轴上厚度为d7,所述摄像光学镜头的光学总长为TTL,且满足下列关系式:
    0.55≤f4/f≤6.42;
    0.57≤(R7+R8)/(R7-R8)≤2.93;
    0.06≤d7/TTL≤0.19。
  7. 根据权利要求1所述的摄像光学镜头,其特征在于,所述第五透镜的焦距为f5,所述第五透镜物侧面的中心曲率半径为R9,所述第五透镜像侧面的中心曲率半径为R10,所述第五透镜的轴上厚度为d9,所述摄像光学镜头的光学总长为TTL,且满足下列关系式:
    -3.13≤f5/f≤-0.51;
    0.74≤(R9+R10)/(R9-R10)≤4.97;
    0.05≤d9/TTL≤0.25。
  8. 根据权利要求1所述的摄像光学镜头,其特征在于,所述摄像光学镜头的光学总长为TTL,所述摄像光学镜头的像高为IH,且满足下列关系式:
    TTL/IH≤1.60。
  9. 根据权利要求1所述的摄像光学镜头,其特征在于,所述摄像光学镜头的视场角为FOV,且满足下列关系式:
    FOV≥77°。
  10. 根据权利要求1所述的摄像光学镜头,其特征在于,所述摄像光学镜头的光圈值为FNO,且满足下列关系式:
    FNO≤2.21。
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