WO2025082012A1 - 一种成像镜头、摄像模组及电子设备 - Google Patents
一种成像镜头、摄像模组及电子设备 Download PDFInfo
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- WO2025082012A1 WO2025082012A1 PCT/CN2024/112886 CN2024112886W WO2025082012A1 WO 2025082012 A1 WO2025082012 A1 WO 2025082012A1 CN 2024112886 W CN2024112886 W CN 2024112886W WO 2025082012 A1 WO2025082012 A1 WO 2025082012A1
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- Prior art keywords
- lens
- imaging
- optical axis
- focal length
- imaging lens
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Classifications
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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
-
- G—PHYSICS
- G02—OPTICS
- G02B—OPTICAL ELEMENTS, SYSTEMS OR APPARATUS
- G02B13/00—Optical objectives specially designed for the purposes specified below
-
- G—PHYSICS
- G02—OPTICS
- G02B—OPTICAL ELEMENTS, SYSTEMS OR APPARATUS
- G02B13/00—Optical objectives specially designed for the purposes specified below
- G02B13/18—Optical objectives specially designed for the purposes specified below with lenses having one or more non-spherical faces, e.g. for reducing geometrical aberration
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- G—PHYSICS
- G03—PHOTOGRAPHY; CINEMATOGRAPHY; ANALOGOUS TECHNIQUES USING WAVES OTHER THAN OPTICAL WAVES; ELECTROGRAPHY; HOLOGRAPHY
- G03B—APPARATUS OR ARRANGEMENTS FOR TAKING PHOTOGRAPHS OR FOR PROJECTING OR VIEWING THEM; APPARATUS OR ARRANGEMENTS EMPLOYING ANALOGOUS TECHNIQUES USING WAVES OTHER THAN OPTICAL WAVES; ACCESSORIES THEREFOR
- G03B17/00—Details of cameras or camera bodies; Accessories therefor
- G03B17/02—Bodies
- G03B17/12—Bodies with means for supporting objectives, supplementary lenses, filters, masks, or turrets
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- G—PHYSICS
- G03—PHOTOGRAPHY; CINEMATOGRAPHY; ANALOGOUS TECHNIQUES USING WAVES OTHER THAN OPTICAL WAVES; ELECTROGRAPHY; HOLOGRAPHY
- G03B—APPARATUS OR ARRANGEMENTS FOR TAKING PHOTOGRAPHS OR FOR PROJECTING OR VIEWING THEM; APPARATUS OR ARRANGEMENTS EMPLOYING ANALOGOUS TECHNIQUES USING WAVES OTHER THAN OPTICAL WAVES; ACCESSORIES THEREFOR
- G03B30/00—Camera modules comprising integrated lens units and imaging units, specially adapted for being embedded in other devices, e.g. mobile phones or vehicles
Definitions
- the present application relates to the field of optical imaging technology, and in particular to an imaging lens, a camera module and an electronic device.
- the thickness of the terminal devices will be gradually reduced, resulting in an increasingly narrow internal space of the terminal devices in the thickness direction.
- a camera module is arranged in the thickness direction of the terminal device, and the narrow internal space of the terminal device in the thickness direction will seriously limit the overall size of the camera module.
- the embodiments of the present application provide an imaging lens, a camera module and an electronic device to solve the problem that the macro and low-light shooting effects of the telephoto lens configured in the mobile terminal are poor.
- an embodiment of the present application provides an imaging lens, which includes a first lens group and a second lens group in sequence from the object side to the image side along the optical axis;
- the first lens group includes a first lens with positive refractive power, a second lens with negative refractive power, and a third lens with positive refractive power in sequence from the object side to the image side along the optical axis;
- the second lens group includes a fourth lens with positive refractive power, a fifth lens with negative refractive power, and a sixth lens with negative refractive power in sequence from the object side to the image side along the optical axis.
- the position of the first lens group is fixed relative to the imaging surface of the camera module; the second lens group is located between the first lens group and the imaging surface, and the second lens group is configured to be movable along the optical axis between the first lens group and the imaging surface; the effective focal length FG1 of the first lens group, the effective focal length FG2 of the second lens group, and the effective focal length Finf of the imaging lens when focusing at infinity satisfy: 1 ⁇ (FG1-FG2)/Finf ⁇ 2.
- the imaging lens by setting the first lens group and the second lens group, and limiting the refractive power of the lenses in the two lens groups, the imaging lens can receive incident light at a larger angle, and converge the aberration and chromatic aberration of the imaging lens, so as to achieve the characteristics of long focus and large aperture and improve the imaging performance of the imaging lens.
- the effective focal length of the first lens group and the second lens group and the effective focal length of the imaging lens when focusing on infinity are designed, so as to improve the imaging quality of the imaging lens at the object distance from infinity to the close focus object distance.
- the object side surface of the first lens is convex at the near optical axis; the object side surface of the second lens is concave at the near optical axis, and the image side surface of the second lens is concave at the near optical axis; the object side surface of the third lens is convex at the near optical axis, and the image side surface of the third lens is convex at the near optical axis; the object side surface of the fourth lens is concave at the near optical axis, and the image side surface of the fourth lens is convex at the near optical axis; the image side surface of the fifth lens is concave at the near optical axis; the object side surface of the sixth lens is concave at the near optical axis, and the image side surface of the sixth lens is concave at the near optical axis.
- the imaging lens can receive incident light at a larger angle, and the light entering the imaging lens can be smoothly transitioned, so that the trend of the light is smoother, thereby realizing the characteristics of large aperture and large target surface, so as to improve the imaging quality of the imaging lens.
- the effective focal length f1 of the first lens satisfies the effective focal length Finf of the imaging lens when focusing at infinity: 0.3 ⁇ f1/Finf ⁇ 1.
- the first lens can also enable the imaging lens to receive incident light at a larger angle, expand the field of view of the imaging lens, and thus achieve the characteristics of a long focal length, a large aperture, and a large target surface.
- the effective focal length f1 of the first lens and the effective focal length f2 of the second lens satisfy: -2.8 ⁇ f1/f2 ⁇ -1.5. In this way, by constraining the effective focal lengths of the first lens and the second lens, the second lens can transition the light incident through the first lens, reduce the bending angle of the light incident at a large angle, balance the coma of the imaging lens, and ensure the imaging performance of the entire system under high and low temperature conditions.
- the effective focal length Finf of the imaging lens when focusing on infinity and the effective focal length Fmac of the imaging lens when focusing on macro satisfy: Finf/Fmac ⁇ 1.5.
- the effective focal length f3 of the third lens and the effective focal length FG1 of the first lens group satisfy: 0.2 ⁇ f3/FG1 ⁇ 1.0.
- the third lens can shrink the light incident through the first lens and the second lens, reduce the deviation of the edge light, thereby balancing the spherical aberration and coma of the imaging lens, and improving the imaging quality of the imaging lens with a long focal length and a large aperture.
- the effective focal length f6 of the sixth lens and the effective focal length FG2 of the second lens group satisfy: 0.5 ⁇ f6/FG2 ⁇ 3. In this way, by constraining the ratio of the effective focal length of the sixth lens to the effective focal length of the second lens group, the field curvature of the imaging lens can be balanced, thereby improving the imaging performance of the imaging lens in a close focus state.
- the center thickness CT4 of the fourth lens on the optical axis, the curvature radius R41 of the object side surface of the fourth lens, and the curvature radius R42 of the image side surface of the fourth lens satisfy: 0.5 ⁇ CT4*(R42/R41) ⁇ 3.
- the shape of the fourth lens can be controlled, the light can be effectively controlled, so as to balance the field curvature and astigmatism, and it is beneficial to realize the characteristics of a large target surface and improve the imaging quality of the imaging lens.
- the curvature radius R32 of the image side surface of the third lens and the curvature radius R41 of the object side surface of the fourth lens satisfy: 0.5 ⁇ R41/R32 ⁇ 5.
- the combined focal length f45 of the fourth lens and the fifth lens and the spatial interval T56 between the fifth lens and the sixth lens on the optical axis satisfy: -100 ⁇ f45/T56 ⁇ -5.
- the second lens group can balance the field curvature and astigmatism, and at the same time, an assembly position can be reserved for the structural parts, so that the imaging lens is conveniently arranged in the terminal device.
- the distance BFLmin between the image side and the imaging surface of the sixth lens in the direction of the optical axis during macro focusing and the distance TTL between the object side and the imaging surface of the first lens in the direction of the optical axis satisfy: BFLmin/TTL>0.05.
- the focusing stroke of the imaging lens can be optimized by constraining the distance between the image side and the imaging surface of the sixth lens in the close focus state, and the structure of the imaging lens can also be optimized to facilitate the arrangement of the voice coil motor structure, thereby realizing the miniaturization of the imaging lens.
- an embodiment of the present application provides a camera module, which includes, from the object side to the image side, an aperture, an imaging lens as described above, and an imaging surface.
- the camera module with the imaging lens has the characteristics of a long focal length, a large aperture, and a large target surface on the basis of a miniaturized structure, thereby improving the imaging performance of the camera module.
- an embodiment of the present application provides an electronic device, comprising a front panel, a middle frame, a back cover, and a camera module as described above, wherein: a display screen is provided on the front panel, the middle frame is provided between the front panel and the back cover, and a camera hole is provided on the back cover; the camera module is provided in the electronic device through the camera hole, and the optical axis direction of the imaging lens in the camera module is parallel to the thickness direction of the electronic device.
- the camera module can be provided in the electronic device, and miniaturization can be achieved through the camera module.
- FIG1 is a schematic diagram of the structure of an electronic device having an electronic camera function in the thickness direction;
- FIG. 2 is a schematic diagram of the internal structure of the camera module 150
- FIG3 is a schematic structural diagram of a camera module 200 provided in an embodiment of the present application.
- FIG4 is a schematic structural diagram of another camera module 200 provided in an embodiment of the present application.
- FIG5 is a schematic diagram of the structure of the imaging lens 210 provided in the first embodiment of the present application when focusing at infinity;
- FIG6 is a schematic diagram of the structure of the imaging lens 210 provided in the first embodiment of the present application when focusing on a macro distance;
- FIG. 7 is an astigmatism curve diagram and a distortion curve diagram of the imaging lens 210 provided in the first embodiment of the present application when focusing at infinity;
- FIG8 is an astigmatism curve diagram and a distortion curve diagram of the imaging lens 210 provided in the first embodiment of the present application when focusing at a macro distance;
- FIG9 is a schematic diagram of the structure of the imaging lens 210 provided in the second embodiment of the present application when focusing at infinity;
- FIG10 is a schematic diagram of the structure of the imaging lens 210 provided in the second embodiment of the present application when focusing on a macro distance;
- FIG. 11 is an astigmatism curve diagram and a distortion curve diagram of the imaging lens 210 provided in the second embodiment of the present application when focusing at infinity;
- FIG. 12 is an astigmatism curve diagram and a distortion curve diagram of the imaging lens 210 provided in the second embodiment of the present application when focusing at a macro distance;
- FIG13 is a schematic diagram of the structure of the imaging lens 210 provided in the third embodiment of the present application when focusing at infinity;
- FIG. 15 is an astigmatism curve diagram and a distortion curve diagram of the imaging lens 210 provided in the third embodiment of the present application when focusing at infinity;
- FIG. 16 is an astigmatism curve diagram and a distortion curve diagram of the imaging lens 210 provided in the third embodiment of the present application when focusing at a macro distance;
- FIG17 is a schematic diagram of the structure of the imaging lens 210 provided in the fourth embodiment of the present application when focusing at infinity;
- FIG18 is a schematic structural diagram of the imaging lens 210 provided in the fourth embodiment of the present application when focusing on a macro distance;
- FIG21 is a schematic diagram of the structure of an imaging lens 210 provided in Embodiment 5 of the present application when focusing at infinity;
- FIG22 is a schematic diagram of the structure of the imaging lens 210 provided in Embodiment 5 of the present application when focusing on a macro distance;
- FIG23 is an astigmatism curve diagram and a distortion curve diagram of the imaging lens 210 provided in Embodiment 5 of the present application when focusing at infinity;
- FIG24 is an astigmatism curve diagram and a distortion curve diagram of the imaging lens 210 provided in Embodiment 5 of the present application when focusing at a macro distance;
- FIG. 25 is a schematic diagram of the structure of the imaging lens 210 provided in Embodiment 6 of the present application when focusing at infinity;
- FIG26 is a schematic diagram of the structure of the imaging lens 210 provided in Embodiment 6 of the present application when focusing on a macro distance;
- FIG27 is an astigmatism curve diagram and a distortion curve diagram of the imaging lens 210 provided in Embodiment 6 of the present application when focusing at infinity;
- FIG29 is a schematic diagram of the structure of an electronic device in the thickness direction according to an embodiment of the present application.
- FIG30 is a schematic diagram of an electronic device in an embodiment of the present application.
- first”, “second”, etc. are used for descriptive purposes only and are not to be understood as indicating or implying relative importance or implicitly indicating the number of the indicated technical features.
- a feature defined as “first”, “second”, etc. may explicitly or implicitly include one or more of the features.
- “plurality” means two or more.
- the thickness, size, proportion and other parameters of the lens are exaggerated. Therefore, the thickness, size, shape and other parameters of the spherical or aspherical surface shown in the drawings are only for illustration and do not represent the actual shape of the aspherical or aspherical surface. In other words, the shape of the spherical or aspherical surface is not limited to the shape of the spherical or aspherical surface shown in the drawings.
- the central area of the lens is the paraxial area, that is, the area near the optical axis.
- the edge area of the lens is the distal area, that is, the area of the lens far from the optical axis. If the surface of the lens is convex and the position of the convex surface is not defined, it means that the surface of the lens is convex at least in the central area. If the surface of the lens is concave and the position of the concave surface is not defined, it means that the surface of the lens is concave at least in the central area.
- camera functions such as smart phones, tablet computers, video cameras, digital cameras, etc., all of which are equipped with camera modules to realize the camera function.
- the present application embodiment is described by taking a smart phone as an example.
- Fig. 1 is a schematic diagram of the structure of an electronic device with an electronic camera function in the thickness direction.
- the electronic device 100 includes a front panel 110, a middle frame 120, a back cover 130, an electronic component 140 and a camera module 150, wherein the front panel 110, the middle frame 120 and the back cover 130 enclose a chamber, and the electronic component 140 and the camera module 150 are arranged in the chamber.
- the camera module 150 may be the front camera and/or the rear camera of the electronic device 100 , and the specific setting position of the camera module 150 is not limited in the present application.
- FIG2 is a schematic diagram of the internal structure of the camera module 150.
- the camera module 150 includes an aperture 151, an imaging lens 152, and an image sensor 153.
- the camera module 150 may also include other imaging-related components, such as a protective film, a voice coil motor (VCM), a filter, a base, a conductive cloth, a rigid-flex board, and a connector, which are not listed here one by one.
- VCM voice coil motor
- the imaging lens 152 In order to meet the user's requirements for the camera function of the electronic device 100, the imaging lens 152 needs to be able to capture images at long distances, macro distances, and The imaging quality is good under dark light conditions.
- the imaging lens 152 can be formed by combining multiple lenses to perform imaging. As shown in FIG2 , the imaging lens 152 includes n lenses 1521 arranged in sequence along the optical axis direction of the imaging lens 152 , where n is a positive integer greater than 1, and the optical axis direction of the imaging lens 152 is the same as the thickness direction of the electronic device 100 .
- the image sensor 153 includes a photosensitive element, such as a charge coupled device (CCD) and a complementary metal oxide semiconductor (CMOS).
- CMOS complementary metal oxide semiconductor
- the image sensor 153 is used to sense the light focused by the imaging lens 152 and form an electronic image corresponding to the scene on the imaging surface, wherein the imaging surface is the surface of the image sensor 153 facing the lens 1521.
- the imaging lens 152 has a higher ability to converge light, which can effectively improve the resolution and contrast of the imaging lens 152, and can also improve the anti-glare effect and imaging quality of the imaging lens 152.
- the thickness of the imaging lens 152 will also be greater.
- the size of the electronic device 100 in the thickness direction will be gradually reduced.
- the size of the camera module 150 in the thickness direction of the electronic device 100 also needs to be reduced, and accordingly, the size of the imaging lens 152 in the thickness direction of the electronic device 100 also needs to be reduced.
- the traditional telephoto lens uses a motor to move the entire lens to achieve focus, which is not conducive to the miniaturization of the camera module 150.
- the focus is achieved by moving the lens with a motor, and the imaging quality of the telephoto lens is very poor at macro distances, and the telephoto macro shooting effect is poor.
- the miniaturized telephoto lens has a small aperture and a small target surface, and the dark light shooting effect is poor.
- the imaging lens 152 includes a sufficient number of lenses 1521 and effectively control the size of the imaging lens 152 in the thickness direction of the electronic device 100. It is also necessary to make a reasonable design for the lenses 1521 in the imaging lens 152, so as to improve its imaging quality in macro or dark light environments.
- FIG. 3 is a schematic diagram of the structure of a camera module 200 provided in an embodiment of the present application
- FIG. 4 is a schematic diagram of the structure of another camera module 200 provided in an embodiment of the present application.
- the camera module 200 includes an aperture ST0, an imaging lens 210, and an imaging surface L8 in sequence from the object side to the image side along the optical axis 201.
- the camera module 200 may further include a filter L7, which is disposed between the imaging lens 210 and the imaging surface L8.
- the imaging lens 210 includes a first lens group 211 and a second lens group 212 in sequence from the object side to the image side along the optical axis 201, wherein the first lens group 211 includes a first lens L1, a second lens L2 and a third lens L3 in sequence from the object side to the image side along the optical axis 201; the second lens group 212 includes a fourth lens L4, a fifth lens L5 and a sixth lens L6 in sequence from the object side to the image side along the optical axis 201.
- the position of the first lens group 211 is fixed relative to the imaging surface L8 of the camera module 200; the second lens group 212 is located between the first lens group 211 and the imaging surface L8, and the second lens group 212 is configured to be movable between the first lens group 211 and the imaging surface L8 along the optical axis 201.
- each lens in the imaging lens 210 has an object side and an image side, wherein the object side refers to the mirror surface in the lens facing the object side, and the image side refers to the mirror surface in the lens facing the image side.
- the first lens L1 includes an object side surface E11 and an image side surface E12
- the second lens L2 includes an object side surface E21 and an image side surface E22
- the third lens L3 includes an object side surface E31 and an image side surface E32
- the fourth lens L4 includes an object side surface E41 and an image side surface E42
- the fifth lens L5 includes an object side surface E51 and an image side surface E52
- the sixth lens L6 includes an object side surface E61 and an image side surface E62.
- the aperture ST0 is disposed between the object side and the imaging lens 210, and in some embodiments, the aperture ST0 is an annular sheet structure capable of blocking light incident from the edge of the imaging lens 210. It should be understood that the aperture ST0 The larger the aperture of the aperture, the higher the light transmittance, and the smaller the aperture of the aperture ST0, the lower the light transmittance.
- the filter L7 also has an object side surface IR1 and an image side surface IR2, and the filter L7 is used to correct color deviation and/or protect the photosensitive element located on the imaging surface L8.
- the filter L7 may include blue glass and/or IR-CUT double filter, etc.
- the specific type of the filter L7 is not limited in the embodiments of the present application.
- the incident light before the incident light enters the imaging lens 210, some edge light will be intercepted by the aperture ST0 and cannot enter the imaging lens 210.
- the incident light that is not intercepted by the aperture ST0 enters from the object side surface E11 of the first lens L1, and then the incident light passes through each subsequent lens in sequence and exits from the image side surface E62 of the sixth lens L6.
- the outgoing light enters from the object side surface IR1 of the filter L7 and exits through the image side surface IR2.
- the outgoing light filtered by the filter L7 is incident on the imaging surface L8, and the imaging surface L8 senses the light and generates a corresponding electronic image.
- the first lens L1 has positive refractive power
- the second lens L2 has negative refractive power
- the third lens L3 has positive refractive power
- the fourth lens L4 has positive refractive power
- the fifth lens L5 has negative refractive power
- the sixth lens L6 has negative refractive power.
- the object-side surface E11 of the first lens L1 is convex at the near optical axis 201
- the image-side surface E12 of the first lens L1 can be convex or concave at the near optical axis 201
- the object-side surface E21 of the second lens L2 is concave at the near optical axis 201
- the image-side surface E22 of the second lens L2 is concave at the near optical axis 201
- the object-side surface E31 of the third lens L3 is convex at the near optical axis 201
- the image-side surface E32 of the third lens L3 is convex surface
- the object-side surface E41 of the fourth lens L4 is concave at the near optical axis 201
- the image-side surface E42 of the fourth lens L4 is convex at the near optical axis 201
- the object-side surface E51 of the fifth lens L5 can be a convex surface or a concave surface at the near optical
- the concavo-convex of the object side of the lens is based on the image side, the object side is curved away from the image side to be convex, and the object side is curved toward the image side to be concave.
- the concavo-convex of the image side of the lens is based on the object side, the image side is curved toward the object side to be concave, and the image side is curved away from the object side to be convex.
- the first lens L1 with positive refractive power can quickly converge the incident light, converge the aperture of the imaging lens 210, and at the same time receive incident light at a larger angle, thereby increasing the field of view of the imaging.
- the third lens L3 with positive refractive power can shrink the incident light and reduce the deviation of the marginal light, thereby balancing the spherical aberration and coma of the imaging lens.
- the fourth lens L4 with positive refractive power can balance the field curvature and astigmatism generated by the imaging lens 210 .
- the fifth lens L5 having negative refractive power can reduce aberrations and chromatic aberrations generated by the imaging lens 210 .
- the sixth lens L6 with negative refractive power can balance aberrations and field curvature and facilitate the smooth transition of light to the imaging surface.
- the effective focal length FG1 of the first lens group 211, the effective focal length FG2 of the second lens group 212, and the effective focal length Finf of the imaging lens 210 when focusing at infinity satisfy the relationship (1): 1 ⁇ (FG1-FG2)/Finf ⁇ 2 (1)
- the effective focal length of the first lens group 211 and the second lens group 212 and the effective focal length of the imaging lens 210 when focusing at infinity By designing the effective focal length of the first lens group 211 and the second lens group 212 and the effective focal length of the imaging lens 210 when focusing at infinity, the imaging quality of the imaging lens from infinite object distance to close focus object distance can be improved, and the situation of different imaging quality when focusing on objects at different distances can be avoided.
- the effective focal length f1 of the first lens L1 and the effective focal length Finf of the imaging lens 210 when focusing at infinity satisfy the relationship (2): 0.3 ⁇ f1/Finf ⁇ 1 (2)
- the effective focal length f1 of the first lens L1 and the effective focal length f2 of the second lens L2 satisfy the relationship (3): -2.8 ⁇ f1/f2 ⁇ -1.5 (3)
- the second lens L2 can transition the light incident through the first lens L1, reduce the bending angle of the light incident at a large angle, balance the coma of the imaging lens 210, and ensure the imaging performance of the entire system under high and low temperature conditions.
- the movement range of the second lens group 212 on the optical axis 201 is limited, and the miniaturization of the imaging lens is achieved on the basis of having higher imaging performance, so that the imaging lens 210 can be used in electronic devices with smaller thickness.
- the effective focal length f3 of the third lens L3 and the effective focal length FG1 of the first lens group 211 satisfy the relationship (5): 0.2 ⁇ f3/FG1 ⁇ 1.0 (5)
- the third lens L3 can shrink the light incident through the first lens L1 and the second lens L2, reduce the deviation of the marginal light, thereby balancing the spherical aberration and coma of the imaging lens 210, and improving the imaging quality of the imaging lens 210 with a long focal length and a large aperture.
- the effective focal length f6 of the sixth lens L6 and the effective focal length FG2 of the second lens group 212 satisfy the relationship (6): 0.5 ⁇ f6/FG2 ⁇ 3 (6)
- the field curvature of the imaging lens 210 can be balanced, thereby improving the imaging performance of the imaging lens 210 in a close focus state.
- a central thickness CT4 of the fourth lens L4 on the optical axis 201, a curvature radius R41 of an object-side surface E41 of the fourth lens L4, and a curvature radius R42 of an image-side surface E42 of the fourth lens L4 satisfy equation (7): 0.5 ⁇ CT4*(R42/R41) ⁇ 3 (7)
- the shape of the fourth lens L4 can be controlled, and the light can be effectively controlled, thereby balancing the field curvature and astigmatism, and it is beneficial to realize the characteristics of a large target surface and improve the imaging quality of the imaging lens 210.
- a curvature radius R32 of the image-side surface E32 of the third lens L3 and a curvature radius R41 of the object-side surface E41 of the fourth lens L4 satisfy equation (8): 0.5 ⁇ R41/R32 ⁇ 5 (8)
- the adjacent lenses in the first lens group 211 and the second lens group 212 can be constrained, so that the light can smoothly enter the second lens group 212 from the first lens group 211, thereby reducing the assembly tolerance sensitivity between the first lens group 211 and the second lens group 212, reducing the assembly difficulty, and improving the imaging quality and assembly processability of the imaging lens 210.
- the combined focal length f45 of the fourth lens L4 and the fifth lens L5, and the spatial interval T56 between the fifth lens L5 and the sixth lens L6 on the optical axis 201 satisfy the relationship (9): -100 ⁇ f45/T56 ⁇ -5 (9)
- the second lens group 212 can balance the field curvature and astigmatism, and at the same time reserve an assembly position for the structural parts, so that the imaging lens 210 is conveniently set in the terminal device.
- the distance BFLmin between the image-side surface E62 of the sixth lens L6 and the imaging surface L8 in the direction of the optical axis 201 and the distance TTL between the object-side surface E11 of the first lens L1 and the imaging surface L8 in the direction of the optical axis 201 satisfy the relationship (10): BFLmin/TTL>0.05 (10)
- the focusing stroke of the imaging lens 210 can be optimized by constraining the distance between the image side surface E62 and the imaging surface L8 when the sixth lens L6 is in a near-focus state.
- the structure of the imaging lens 210 can also be optimized to facilitate the arrangement of the voice coil motor structure, thereby realizing the miniaturization of the imaging lens 210.
- each lens includes at least one aspherical lens, that is, at least one mirror surface from the object side surface E11 of the first lens L1 to the image side surface E62 of the sixth lens L6 is an aspherical mirror surface.
- the aspherical lens has the characteristic of continuously changing curvature from the center of the lens to the edge of the lens. Unlike a spherical lens with a constant curvature from the center of the lens to the edge of the lens, the aspherical lens has a better curvature radius characteristic and has the advantage of improving aberrations. After using an aspherical lens, the aberrations that occur during imaging can be eliminated as much as possible, thereby improving the imaging quality.
- At least one of the object-side surface and the image-side surface of each of the first lens L1, the second lens L2, the third lens L3, the fourth lens L4, the fifth lens L5 and the sixth lens L6 is an aspherical mirror surface.
- the object-side surface and the image-side surface of each of the first lens L1, the second lens L2, the third lens L3, the fourth lens L4, the fifth lens L5 and the sixth lens L6 are aspherical mirror surfaces.
- each lens includes at least one glass lens.
- the first lens L1 in the imaging lens 210 may be a glass lens, and the rest may be plastic lenses.
- glass lenses have a lower dispersion coefficient on the basis of a higher refractive index, so that the first lens L1 can reduce its temperature sensitivity while having good optical performance, so that the imaging lens 210 can be used in more environments.
- the above-mentioned lens material is only an exemplary description in this application, and the specific material composition of each lens is not limited in this application.
- the imaging lens 210 provided in the embodiment of the present application can not only increase the amount of light entering the lens and enhance the image quality in a dark environment, but also avoid adverse effects such as overexposure in a bright environment.
- the incident light can be effectively converged, and aberrations and astigmatism can be reduced, so that the imaging lens 210 can adapt to the size of the terminal device in the thickness direction, and the imaging quality of the imaging lens 210 in a complex light environment can be effectively improved, and the convenience of processing and assembly of each lens can be effectively improved.
- the camera module 200 provided in the embodiment of the present application can also have the characteristics of long focal length, large aperture, large target surface and high imaging quality on the basis of adapting to the size of the terminal device in the thickness direction.
- imaging lens 210 Some optional embodiments of the imaging lens 210 will be described in detail below in combination with specific parameters.
- FIG5 is a schematic diagram of the structure of the imaging lens 210 provided in the first embodiment of the present application when focusing on infinity
- FIG6 is a schematic diagram of the structure of the imaging lens 210 provided in the first embodiment of the present application when focusing on macro.
- the camera module 200 includes, from the object side to the image side along the optical axis 201, an aperture ST0, a first lens group 211, a second lens group 212, a filter L7, and an imaging surface L8.
- the first lens group 211 includes, from the object side to the image side along the optical axis 201, a first lens L1, a second lens L2, and a third lens L3, and the second lens group 212 includes, from the object side to the image side along the optical axis 201, a fourth lens L4, a fifth lens L5, and a sixth lens L6.
- the first lens L1 has positive refractive power, an object-side surface E11 of the first lens L1 is convex at the near optical axis 201, and an image-side surface E12 of the first lens L1 is concave at the near optical axis 201.
- the second lens L2 has negative refractive power, an object-side surface E21 of the second lens L2 is concave at the near optical axis 201, and an image-side surface E22 of the second lens L2 is concave at the near optical axis 201.
- the third lens L3 has positive refractive power, an object-side surface E31 of the third lens L3 is convex at the near optical axis 201, and an image-side surface E32 of the third lens L3 is convex at the near optical axis 201.
- the fourth lens L4 has positive refractive power, an object-side surface E41 of the fourth lens L4 is concave at the near optical axis 201, and an image-side surface E42 of the fourth lens L4 is convex at the near optical axis 201.
- the fifth lens L5 has negative refractive power, an object-side surface E51 of the fifth lens L5 is convex at the near optical axis 201, and an image-side surface E52 of the fifth lens L5 is concave at the near optical axis 201.
- the sixth lens L6 has negative refractive power, an object-side surface E61 of the sixth lens L6 is concave at the near optical axis 201, and an image-side surface E62 of the sixth lens L6 is concave at the near optical axis 201.
- the value corresponding to the object side of the lens and the filter is the central thickness of the lens or the filter, that is, the thickness of the lens or the filter on the optical axis 201; and the value corresponding to the image side of the lens and the filter is the spatial interval between the lens or the filter and the object side of the rear component on the optical axis 201.
- the effective focal length Finf of the imaging lens 210 when focusing on infinity is 18.6 mm
- the effective focal length Fmac of the imaging lens 210 when focusing on macro is 13.95 mm.
- the F number FNOinf of the imaging lens 210 when focusing on infinity is 1.93
- the F number FNOmac of the imaging lens 210 when focusing on macro is 1.48.
- the field of view FOVinf of the imaging lens 210 when focusing on infinity is 17.22°
- the field of view FOVmac of the imaging lens 210 when focusing on macro is 18.08°.
- the effective focal length FG1 of the first lens group 211 is 12.31 mm
- the effective focal length FG2 of the second lens group 212 is -12.14 mm.
- the incident light is intercepted by the aperture ST0 as shown in FIG5 and FIG6 , and a portion of the light is retained to enter from the object side surface E11 of the first lens L1, and the incident light passes through each lens in sequence and is emitted from the image side surface E62 of the sixth lens L6.
- the outgoing light enters from the object side surface IR1 of the filter L7 and is emitted through the image side surface IR2.
- the outgoing light filtered by the filter L7 is incident on the imaging surface L8, and the imaging surface L8 senses the incident light and generates a corresponding electronic image.
- Fig. 7 is an astigmatism curve and a distortion curve of the imaging lens 210 provided in the first embodiment of the present application when focusing at infinity.
- Fig. 8 is an astigmatism curve and a distortion curve of the imaging lens 210 provided in the first embodiment of the present application when focusing at macro.
- FIG9 is a schematic diagram of the structure of the imaging lens 210 provided in the second embodiment of the present application when focusing on infinity
- FIG10 is a schematic diagram of the structure of the imaging lens 210 provided in the second embodiment of the present application when focusing on macro.
- the camera module 200 includes: an aperture ST0, a first lens group 211, a second lens group 212, a filter L7, and an imaging surface L8 in sequence from the object side to the image side along the optical axis 201.
- the first lens group 211 includes a first lens L1, a second lens L2, and a third lens L3 in sequence from the object side to the image side along the optical axis 201
- the second lens group 212 includes a fourth lens L4, a fifth lens L5, and a sixth lens L6 in sequence from the object side to the image side along the optical axis 201.
- the first lens L1 has positive refractive power, an object-side surface E11 of the first lens L1 is convex at the near optical axis 201, and an image-side surface E12 of the first lens L1 is concave at the near optical axis 201.
- the second lens L2 has negative refractive power, an object-side surface E21 of the second lens L2 is concave at the near optical axis 201, and an image-side surface E22 of the second lens L2 is concave at the near optical axis 201.
- the third lens L3 has positive refractive power, an object-side surface E31 of the third lens L3 is convex at the near optical axis 201, and an image-side surface E32 of the third lens L3 is convex at the near optical axis 201.
- the fourth lens L4 has positive refractive power, an object-side surface E41 of the fourth lens L4 is concave at the near optical axis 201, and an image-side surface E42 of the fourth lens L4 is convex at the near optical axis 201.
- the fifth lens L5 has negative refractive power
- the object-side surface E51 of the fifth lens L5 is convex at the near optical axis 201
- the image-side surface E52 of the fifth lens L5 is concave at the near optical axis 201.
- the sixth lens L6 has negative refractive power
- the object-side surface E61 of the sixth lens L6 is concave at the near optical axis 201
- the image-side surface E62 of the sixth lens L6 is concave at the near optical axis 201.
- Table 3 shows basic parameters of the camera module 200 of the second embodiment, wherein the units of the curvature radius, thickness and focal length are all millimeters (mm).
- the thickness values listed in Table 3 correspond to the values on the side of the lens and filter. or the center thickness of the filter, that is, the thickness of the lens or filter on the optical axis 201; and the value corresponding to the image side of the lens or filter is the spatial interval between the lens or filter and the object side of the rear component on the optical axis 201.
- the spatial distance T34 between the image side surface E32 of the third lens L3 and the object side surface E41 of the fourth lens L4 is 0.6 mm
- the spatial distance T67 between the image side surface E62 of the sixth lens L6 and the object side surface IR1 of the filter L7 is 3.93 mm.
- the spatial distance T34 between the image side surface E32 of the third lens L3 and the object side surface E41 of the fourth lens L4 is 3.48 mm
- the spatial distance T67 between the image side surface E62 of the sixth lens L6 and the object side surface IR1 of the filter L7 is 1.05 mm.
- the effective focal length Finf of the imaging lens 210 when focusing on infinity is 19.95 mm
- the effective focal length Fmac of the imaging lens 210 when focusing on macro is 15.10 mm
- the F number FNOinf of the imaging lens 210 when focusing on infinity is 1.96
- the F number FNOmac of the imaging lens 210 when focusing on macro is 1.52.
- the field of view FOVinf of the imaging lens 210 when focusing on infinity is 17.2°
- the field of view FOVmac of the imaging lens 210 when focusing on macro is 18.05°.
- the effective focal length FG1 of the first lens group 211 is 13.66 mm
- the effective focal length FG2 of the second lens group 212 is -12.65 mm.
- the distance between the lens and the object plane is less than or equal to 13 cm.
- Example 2 the object side surface and the image side surface of any lens among the first lens L1 to the sixth lens L6 are aspherical surfaces, and the surface shape of each aspherical lens satisfies the formula (11) in Example 1.
- Tables 4-1 and 4-2 show the high-order coefficients of each aspherical mirror surface that can be used in Example 2.
- the incident light is intercepted by the aperture ST0 as shown in Figures 9 and 10, and part of the light is retained from the object lens of the first lens L1.
- the incident light enters from the side surface E11, passes through each lens in sequence, and is emitted from the image side surface E62 of the sixth lens L6.
- the outgoing light enters from the object side surface IR1 of the filter L7 and is emitted through the image side surface IR2.
- the outgoing light filtered by the filter L7 is incident on the imaging surface L8, and the imaging surface L8 senses the incident light and generates a corresponding electronic image.
- Fig. 11 is an astigmatism curve and a distortion curve of the imaging lens 210 provided in the second embodiment of the present application when focusing at infinity.
- Fig. 12 is an astigmatism curve and a distortion curve of the imaging lens 210 provided in the second embodiment of the present application when focusing at macro.
- the astigmatism curve is used to represent the meridional image curvature and the sagittal image curvature
- the distortion curve is used to represent the distortion magnitude values corresponding to different image heights.
- the wavelength of the reference light used for testing is 555nm. According to Figures 11 and 12, at this reference wavelength, the imaging lens 210 provided in the second embodiment can well compensate and correct the astigmatism and distortion, so that the imaging lens 210 can achieve good imaging quality.
- FIG13 is a schematic diagram of the structure of the imaging lens 210 provided in the third embodiment of the present application when focusing on infinity
- FIG14 is a schematic diagram of the structure of the imaging lens 210 provided in the third embodiment of the present application when focusing on macro.
- the camera module 200 includes: an aperture ST0, a first lens group 211, a second lens group 212, a filter L7, and an imaging surface L8 in sequence from the object side to the image side along the optical axis 201.
- the first lens group 211 includes a first lens L1, a second lens L2, and a third lens L3 in sequence from the object side to the image side along the optical axis 201
- the second lens group 212 includes a fourth lens L4, a fifth lens L5, and a sixth lens L6 in sequence from the object side to the image side along the optical axis 201.
- the first lens L1 has positive refractive power, an object-side surface E11 of the first lens L1 is convex at the near optical axis 201, and an image-side surface E12 of the first lens L1 is concave at the near optical axis 201.
- the second lens L2 has negative refractive power, an object-side surface E21 of the second lens L2 is concave at the near optical axis 201, and an image-side surface E22 of the second lens L2 is concave at the near optical axis 201.
- the third lens L3 has positive refractive power, an object-side surface E31 of the third lens L3 is convex at the near optical axis 201, and an image-side surface E32 of the third lens L3 is convex at the near optical axis 201.
- the fourth lens L4 has positive refractive power, an object-side surface E41 of the fourth lens L4 is concave at the near optical axis 201, and an image-side surface E42 of the fourth lens L4 is convex at the near optical axis 201.
- the fifth lens L5 has negative refractive power
- the object-side surface E51 of the fifth lens L5 is convex at the near optical axis 201
- the image-side surface E52 of the fifth lens L5 is concave at the near optical axis 201.
- the sixth lens L6 has negative refractive power
- the object-side surface E61 of the sixth lens L6 is concave at the near optical axis 201
- the image-side surface E62 of the sixth lens L6 is concave at the near optical axis 201.
- Table 5 shows basic parameters of the camera module 200 of the third embodiment, wherein the units of the radius of curvature, thickness and focal length are all millimeters (mm).
- the value corresponding to the object side of the lens and the filter is the central thickness of the lens or the filter, that is, the thickness of the lens or the filter on the optical axis 201; and the value corresponding to the image side of the lens and the filter is the spatial interval between the lens or the filter and the object side of the rear component on the optical axis 201.
- the spatial distance T34 between the image side surface E32 of the third lens L3 and the object side surface E41 of the fourth lens L4 is 0.6 mm
- the spatial distance T67 between the image side surface E62 of the sixth lens L6 and the object side surface IR1 of the filter L7 is 4.04 mm.
- the spatial distance T34 between the image side surface E32 of the third lens L3 and the object side surface E41 of the fourth lens L4 is 3.47 mm
- the spatial distance T67 between the image side surface E62 of the sixth lens L6 and the object side surface IR1 of the filter L7 is 1.17 mm.
- the effective focal length Finf of the imaging lens 210 when focusing on infinity is 19.98 mm
- the effective focal length Fmac of the imaging lens 210 when focusing on macro is 15.03 mm.
- the F number FNOinf of the imaging lens 210 when focusing on infinity is 1.93
- the F number FNOmac of the imaging lens 210 when focusing on macro is 1.48.
- the field of view FOVinf of the imaging lens 210 when focusing on infinity is 17.18°
- the field of view FOVmac of the imaging lens 210 when focusing on macro is 17.99°
- the effective focal length FG1 of the first lens group 211 is 13.40 mm
- the effective focal length FG2 of the second lens group 212 is -13.14 mm.
- the distance between the lens and the object plane is less than or equal to 13 cm.
- Example 3 the object side surface and the image side surface of any lens among the first lens L1 to the sixth lens L6 are aspherical surfaces, and the surface shape of each aspherical lens satisfies the formula (11) in Example 1.
- Tables 6-1 and 6-2 show the high-order coefficients of each aspherical mirror surface that can be used in Example 3.
- the incident light is intercepted by the aperture ST0 as shown in FIG. 13 and FIG. 14 , and a portion of the light is retained to enter from the object side surface E11 of the first lens L1.
- the incident light passes through each lens in sequence and is emitted from the image side surface E62 of the sixth lens L6.
- the outgoing light enters from the object side surface IR1 of the filter L7 and is emitted through the image side surface IR2.
- the outgoing light filtered by the filter L7 is incident on the imaging surface L8, and the imaging surface L8 senses the incident light and generates a corresponding electronic image.
- Fig. 15 is an astigmatism curve and a distortion curve of the imaging lens 210 provided in the third embodiment of the present application when focusing on infinity.
- Fig. 16 is an astigmatism curve and a distortion curve of the imaging lens 210 provided in the third embodiment of the present application when focusing on macro.
- the astigmatism curve is used to represent the meridional image curvature and the sagittal image curvature
- the distortion curve is used to represent the distortion magnitude values corresponding to different image heights.
- the wavelength of the reference light used for testing is 555nm. According to Figures 15 and 16, at this reference wavelength, the imaging lens 210 provided in the third embodiment can well compensate and correct the astigmatism and distortion, so that the imaging lens 210 can achieve good imaging quality.
- FIG17 is a schematic diagram of the structure of the imaging lens 210 provided in the fourth embodiment of the present application when focusing on infinity
- FIG18 is a schematic diagram of the structure of the imaging lens 210 provided in the fourth embodiment of the present application when focusing on macro.
- the camera module 200 includes: an aperture ST0, a first lens group 211, a second lens group 212, a filter L7, and an imaging surface L8 in sequence from the object side to the image side along the optical axis 201.
- the first lens L1 has positive refractive power, an object-side surface E11 of the first lens L1 is convex at the near optical axis 201, and an image-side surface E12 of the first lens L1 is convex at the near optical axis 201.
- the second lens L2 has negative refractive power, an object-side surface E21 of the second lens L2 is concave at the near optical axis 201, and an image-side surface E22 of the second lens L2 is concave at the near optical axis 201.
- the third lens L3 has positive refractive power, an object-side surface E31 of the third lens L3 is convex at the near optical axis 201, and an image-side surface E32 of the third lens L3 is convex at the near optical axis 201.
- the fourth lens L4 has positive refractive power, an object-side surface E41 of the fourth lens L4 is concave at the near optical axis 201, and an image-side surface E42 of the fourth lens L4 is convex at the near optical axis 201.
- the fifth lens L5 has negative refractive power
- the object-side surface E51 of the fifth lens L5 is concave at the near optical axis 201
- the image-side surface E52 of the fifth lens L5 is concave at the near optical axis 201.
- the sixth lens L6 has negative refractive power
- the object-side surface E61 of the sixth lens L6 is concave at the near optical axis 201
- the image-side surface E62 of the sixth lens L6 is concave at the near optical axis 201.
- Table 7 shows basic parameters of the camera module 200 of the fourth embodiment, wherein the units of the radius of curvature, thickness and focal length are all millimeters (mm).
- the value corresponding to the object side of the lens and the filter is the central thickness of the lens or the filter, that is, the thickness of the lens or the filter on the optical axis 201; and the value corresponding to the image side of the lens and the filter is the spatial interval between the lens or the filter and the object side of the rear component on the optical axis 201.
- the spatial distance T34 between the image side surface E32 of the third lens L3 and the object side surface E41 of the fourth lens L4 is 0.6 mm
- the spatial distance T67 between the image side surface E62 of the sixth lens L6 and the object side surface IR1 of the filter L7 is 3.88 mm
- the spatial distance T34 between the image side surface E32 of the third lens L3 and the object side surface E41 of the fourth lens L4 is 3.29 mm
- the spatial distance T67 between the image side surface E62 of the sixth lens L6 and the object side surface IR1 of the filter L7 is 1.19 mm.
- the effective focal length Finf of the imaging lens 210 when focusing on infinity is 18.6 mm
- the effective focal length Fmac of the imaging lens 210 when focusing on macro is 13.67 mm.
- the F number FNOinf of the imaging lens 210 when focusing on infinity is 1.90
- the F number FNOmac of the imaging lens 210 when focusing on macro is 1.50.
- the field of view FOVinf of the imaging lens 210 when focusing on infinity is 17.19°
- the field of view FOVmac of the imaging lens 210 when focusing on macro is 18.16°
- the effective focal length FG1 of the first lens group 211 is 12.25 mm
- the effective focal length FG2 of the second lens group 212 is -11.33 mm.
- the distance between the lens and the object plane is less than or equal to 12 cm.
- Example 4 the object side surface and the image side surface of any lens among the first lens L1 to the sixth lens L6 are aspherical surfaces, and the surface shape of each aspherical lens satisfies the formula (11) in Example 1.
- Tables 8-1 and 8-2 show the high-order coefficients of each aspherical mirror surface that can be used in Example 4.
- the incident light is intercepted by the aperture ST0 as shown in FIG17 and FIG18 , and a portion of the light is retained to enter from the object side surface E11 of the first lens L1.
- the incident light passes through each lens in sequence and is emitted from the image side surface E62 of the sixth lens L6.
- the outgoing light enters from the object side surface IR1 of the filter L7 and is emitted through the image side surface IR2.
- the outgoing light filtered by the filter L7 is incident on the imaging surface L8, and the imaging surface L8 senses the incident light and generates a corresponding electronic image.
- Figure 19 is an astigmatism curve and a distortion curve diagram of the imaging lens 210 provided in the fourth embodiment of the present application when focusing on infinity.
- Figure 20 is an astigmatism curve and a distortion curve diagram of the imaging lens 210 provided in the fourth embodiment of the present application when focusing on macro.
- the astigmatism curve is used to represent the meridional image curvature and the sagittal image curvature
- the distortion curve is used to represent the distortion magnitude values corresponding to different image heights.
- the wavelength of the reference light used for testing is 555nm. According to Figures 19 and 20, at this reference wavelength, the imaging lens 210 provided in the fourth embodiment can well compensate and correct the astigmatism and distortion, so that the imaging lens 210 can achieve good imaging quality.
- FIG21 is a schematic diagram of the structure of the imaging lens 210 provided in the fifth embodiment of the present application when focusing on infinity
- FIG22 is a schematic diagram of the structure of the imaging lens 210 provided in the fifth embodiment of the present application when focusing on macro.
- the camera module 200 includes, from the object side to the image side along the optical axis 201, an aperture ST0, a first lens group 211, a second lens group 212, a filter L7, and an imaging surface L8.
- the first lens group 211 includes, from the object side to the image side along the optical axis 201, a first lens L1, a second lens L2, and a third lens L3, and the second lens group 212 includes, from the object side to the image side along the optical axis 201, a fourth lens L4, a fifth lens L5, and a sixth lens L6.
- the first lens L1 has positive refractive power, an object-side surface E11 of the first lens L1 is convex at the near optical axis 201, and an image-side surface E12 of the first lens L1 is convex at the near optical axis 201.
- the second lens L2 has negative refractive power, an object-side surface E21 of the second lens L2 is concave at the near optical axis 201, and an image-side surface E22 of the second lens L2 is concave at the near optical axis 201.
- the third lens L3 has positive refractive power, an object-side surface E31 of the third lens L3 is convex at the near optical axis 201, and an image-side surface E32 of the third lens L3 is convex at the near optical axis 201.
- the fourth lens L4 has positive refractive power, an object-side surface E41 of the fourth lens L4 is concave at the near optical axis 201, and an image-side surface E42 of the fourth lens L4 is convex at the near optical axis 201.
- the fifth lens L5 has negative refractive power
- the object-side surface E51 of the fifth lens L5 is concave at the near optical axis 201
- the image-side surface E52 of the fifth lens L5 is concave at the near optical axis 201.
- the sixth lens L6 has negative refractive power
- the object-side surface E61 of the sixth lens L6 is concave at the near optical axis 201
- the image-side surface E62 of the sixth lens L6 is concave at the near optical axis 201.
- Table 9 shows basic parameters of the camera module 200 of the fifth embodiment, wherein the units of the curvature radius, thickness and focal length are all millimeters (mm).
- the value corresponding to the object side of the lens and the filter is the central thickness of the lens or the filter, that is, the thickness of the lens or the filter on the optical axis 201; and the value corresponding to the image side of the lens and the filter is the spatial interval between the lens or the filter and the object side of the rear component on the optical axis 201.
- the spatial distance T34 between the image side surface E32 of the third lens L3 and the object side surface E41 of the fourth lens L4 is 0.55 mm
- the spatial distance T67 between the image side surface E62 of the sixth lens L6 and the object side surface IR1 of the filter L7 is 3.65 mm.
- the spatial distance T34 between the image side surface E32 of the third lens L3 and the object side surface E41 of the fourth lens L4 is 2.83 mm
- the spatial distance T67 between the image side surface E62 of the sixth lens L6 and the object side surface IR1 of the filter L7 is 1.37 mm.
- the effective focal length Finf of the imaging lens 210 when focusing on infinity is 18.55 mm
- the effective focal length Fmac of the imaging lens 210 when focusing on macro is 14.15 mm.
- the F number FNOinf of the imaging lens 210 when focusing on infinity is 1.88
- the F number FNOmac of the imaging lens 210 when focusing on macro is 1.47.
- the field of view FOVinf of the imaging lens 210 when focusing on infinity is 17.22°
- the field of view FOVmac of the imaging lens 210 when focusing on macro is 17.86°.
- the effective focal length FG1 of the first lens group 211 is 12.08
- the effective focal length FG2 of the second lens group 212 is -11.24.
- the distance between the lens and the object plane is less than or equal to 13 cm.
- Example 5 the object side surface and the image side surface of any lens among the first lens L1 to the sixth lens L6 are aspherical surfaces, and the surface shape of each aspherical lens satisfies the formula (11) in Example 1.
- Tables 10-1 and 10-2 show the high-order coefficients of each aspherical mirror surface that can be used in Example 5.
- the incident light is intercepted by the aperture ST0 as shown in FIG. 21 and FIG. 22, and a portion of the light is retained to enter from the object side surface E11 of the first lens L1.
- the incident light passes through each lens in sequence and is emitted from the image side surface E62 of the sixth lens L6.
- the outgoing light enters from the object side surface IR1 of the filter L7 and is emitted through the image side surface IR2.
- the outgoing light filtered by the filter L7 is incident on the imaging surface L8, and the imaging surface L8 senses the incident light and generates a corresponding electronic image.
- Figure 23 is an astigmatism curve and a distortion curve diagram of the imaging lens 210 provided in the fifth embodiment of the present application when focusing on infinity.
- Figure 24 is an astigmatism curve and a distortion curve diagram of the imaging lens 210 provided in the fifth embodiment of the present application when focusing on macro.
- the astigmatism curve is used to represent the meridional image curvature and the sagittal image curvature
- the distortion curve is used to represent the distortion magnitude values corresponding to different image heights.
- the wavelength of the reference light used for testing is 555nm. According to Figures 23 and 24, at this reference wavelength, the imaging lens 210 provided in Example 5 can well compensate and correct the astigmatism and distortion, so that the imaging lens 210 can achieve good imaging quality.
- FIG25 is a schematic diagram of the structure of the imaging lens 210 provided in Example 6 of the present application when focusing on infinity
- FIG26 is a schematic diagram of the structure of the imaging lens 210 provided in Example 6 of the present application when focusing on macro.
- the camera module 200 includes, from the object side to the image side along the optical axis 201, an aperture ST0, a first lens group 211, a second lens group 212, a filter L7, and an imaging surface L8.
- the first lens group 211 includes, from the object side to the image side along the optical axis 201, a first lens L1, a second lens L2, and a third lens L3, and the second lens group 212 includes, from the object side to the image side along the optical axis 201, a fourth lens L4, a fifth lens L5, and a sixth lens L6.
- the first lens L1 has positive refractive power, the object side surface E11 of the first lens L1 is convex at the near optical axis 201, and the image side surface E12 of the first lens L1 is concave at the near optical axis 201.
- the second lens L2 has negative refractive power, the object side surface E21 of the second lens L2 is concave at the near optical axis 201, and the image side surface E22 of the second lens L2 is concave at the near optical axis 201.
- the third lens L3 has positive refractive power, the object side surface E31 of the third lens L3 is convex at the near optical axis 201, and the image side surface E32 of the third lens L3 is convex at the near optical axis 201.
- the fourth lens L4 has positive refractive power, the object side surface E21 of the fourth lens L4 is concave at the near optical axis 201, and the image side surface E22 of the second lens L2 is concave at the near optical axis 201.
- the surface E41 is concave at the near optical axis 201, and the image-side surface E42 of the fourth lens L4 is convex at the near optical axis 201.
- the fifth lens L5 has negative refractive power
- the object-side surface E51 of the fifth lens L5 is convex at the near optical axis 201
- the image-side surface E52 of the fifth lens L5 is concave at the near optical axis 201.
- the sixth lens L6 has negative refractive power
- the object-side surface E61 of the sixth lens L6 is concave at the near optical axis 201
- the image-side surface E62 of the sixth lens L6 is concave at the near optical axis 201.
- Table 11 shows the basic parameters of the camera module 200 of the sixth embodiment, wherein the units of the curvature radius, thickness and focal length are all millimeters (mm).
- the value corresponding to the object side of the lens and the filter is the central thickness of the lens or the filter, that is, the thickness of the lens or the filter on the optical axis; and the value corresponding to the image side of the lens and the filter is the spatial interval between the lens or the filter and the object side of the rear component on the optical axis 201.
- the spatial distance T34 between the image side surface E32 of the third lens L3 and the object side surface E41 of the fourth lens L4 is 0.56 mm
- the spatial distance T67 between the image side surface E62 of the sixth lens L6 and the object side surface IR1 of the filter L7 is 3.93 mm.
- the spatial distance T34 between the image side surface E32 of the third lens L3 and the object side surface E41 of the fourth lens L4 is 3.28 mm
- the spatial distance T67 between the image side surface E62 of the sixth lens L6 and the object side surface IR1 of the filter L7 is 1.21 mm.
- the effective focal length Finf of the imaging lens 210 when focusing on infinity is 18.6 mm
- the effective focal length Fmac of the imaging lens 210 when focusing on macro is 13.96 mm.
- the F number FNOinf of the imaging lens 210 when focusing on infinity is 1.92
- the F number FNOmac of the imaging lens 210 when focusing on macro is 1.47.
- the field of view FOVinf of the imaging lens 210 when focusing on infinity is 17.21°
- the field of view FOVmac of the imaging lens 210 when focusing on macro is 18.1°.
- the effective focal length FG1 of the first lens group 211 is 12.34 mm
- the effective focal length FG2 of the second lens group 212 is -12.32 mm.
- the distance between the lens and the object plane is less than or equal to 13 cm.
- Example 6 the object side surface and the image side surface of any lens among the first lens L1 to the sixth lens L6 are aspherical surfaces, and the surface shape of each aspherical lens satisfies the formula (11) in Example 1.
- Tables 12-1 and 12-2 show the high-order coefficients of each aspherical mirror surface that can be used in Example 6.
- the incident light is intercepted by the aperture ST0 as shown in FIG25 and FIG26, and a portion of the light is retained to enter from the object side surface E11 of the first lens L1.
- the incident light passes through each lens in sequence and is emitted from the image side surface E62 of the sixth lens L6.
- the outgoing light enters from the object side surface IR1 of the filter L7 and is emitted through the image side surface IR2.
- the outgoing light filtered by the filter L7 is incident on the imaging surface L8, and the imaging surface L8 senses the incident light and generates a corresponding electronic image.
- Figure 27 is an astigmatism curve and a distortion curve diagram of the imaging lens 210 provided in the sixth embodiment of the present application when focusing on infinity.
- Figure 28 is an astigmatism curve and a distortion curve diagram of the imaging lens 210 provided in the sixth embodiment of the present application when focusing on macro.
- the astigmatism curve is used to represent the meridional image curvature and the sagittal image curvature
- the distortion curve is used to represent the distortion magnitude values corresponding to different image heights.
- the wavelength of the reference light used for testing is 546nm. According to Figures 27 and 28, at this reference wavelength, the imaging lens 210 provided in Example 6 can well compensate and correct the astigmatism and distortion, so that the imaging lens 210 can achieve good imaging quality.
- embodiments 1 to 6 respectively satisfy the above-mentioned equations (1) to (10).
- Figure 29 is a schematic diagram of the structure of an electronic device in the thickness direction in an embodiment of the present application
- Figure 30 is a schematic diagram of an electronic device in an embodiment of the present application.
- the present application also provides an electronic device, as shown in Figures 29 and 30, the electronic device includes a front panel 310, a middle frame 320, a back cover 330 and a camera module 200 including any of the aforementioned imaging lenses, wherein a display screen 311 is provided on the front panel 310, the middle frame 320 is arranged between the front panel 310 and the back cover 330, and a camera hole 331 is provided on the back cover 330, the camera module 200 is arranged in the electronic device through the camera hole 331, and the optical axis 201 of the imaging lens in the camera module 200 is parallel to the thickness direction of the electronic device.
- the cavity formed by the front panel 310, the middle frame 320 and the back cover 330 also includes electronic components 340, and the electronic components 340 include but are not limited to processors, antennas, sensors, gyroscopes, speakers and other devices, so that the electronic device can display images or videos obtained by the camera module 200 through the display screen 311.
- the camera module 200 set in the electronic device through the camera hole 331 on the back cover 330 can serve as a rear camera of the electronic device to receive incident light located on the side of the back cover 330 away from the front panel 310 to generate a corresponding electronic image.
- the camera module 200 can also be used as a front camera of the electronic device.
- a camera hole can be set on the front panel 310 of the electronic device, and the camera module 200 can be installed through the camera hole on the front panel 310, so as to receive incident light on the side of the front panel 310 away from the rear cover 330 to generate a corresponding electronic image.
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Abstract
本申请提供了一种成像镜头、摄像模组及电子设备,该成像镜头沿光轴从物侧至像侧依次包括第一透镜组和第二透镜组,其中第一透镜组包括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,第二透镜组包括具有正屈折力的第四透镜、具有负屈折力的第五透镜、具有负屈折力的第六透镜。第一透镜组的位置相对于摄像模组的成像面固定,第二透镜组位于第一透镜组与成像面之间,第二透镜组可沿光轴在第一透镜组与成像面之间移动,且该成像镜头满足1<(FG1-FG2)/Finf<2。本申请提供的成像镜头、摄像模组及电子设备,能够实现长焦大光圈、大靶面的特征,并提高成像镜头在不同环境及条件下的拍摄质量。
Description
本申请要求于2023年10月18日提交到国家知识产权局、申请号为202311351973.5、发明名称为“一种成像镜头、摄像模组及电子设备”的中国专利申请的优先权,其全部内容通过引用结合在本申请中。
本申请涉及光学成像技术领域,尤其涉及一种成像镜头、摄像模组及电子设备。
随着摄像设备技术的发展,越来越多的移动终端设备具备摄像功能。用户对于移动终端的摄像功能的要求也逐渐多元化,期望移动终端能够实现在远景、微距及暗光场景中均具有良好的拍摄效果。
对于移动终端设备,例如手机,为了更加便于用户携带和使用终端设备,以及提高终端设备的美观度,会逐渐缩小终端设备的厚度,并导致终端设备在厚度方向上的内部空间愈发狭小。通常,在终端设备的厚度方向上配置摄像模组,终端设备在厚度方向上狭小的内部空间将严重限制摄像模组的整体尺寸。
而为了实现在远景、微距及暗光场景中均具有良好的摄影效果,需要通过长焦镜头等摄像模组进行成像。传统的长焦镜头通过马达移动镜头整体来实现对焦,不利于摄像模组的小型化,且通过马达移动镜头实现对焦,在微距时长焦镜头的成像质量很差,长焦微距拍摄效果较差。同时受限于移动终端中模组体积的要求,长焦镜头的光圈较小、靶面较小,暗光拍摄效果差。
发明内容
本申请实施例提供了一种成像镜头、摄像模组及电子设备,以解决配置在移动终端中的长焦镜头微距及暗光拍摄效果差的问题。
第一方面,本申请实施例提供一种成像镜头,沿光轴从物侧至像侧依次包括第一透镜组和第二透镜组;第一透镜组沿光轴从物侧至像侧依次包括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;第二透镜组沿光轴从物侧至像侧依次包括具有正屈折力的第四透镜、具有负屈折力的第五透镜、具有负屈折力的第六透镜。
其中,第一透镜组的位置相对于摄像模组的成像面固定;第二透镜组位于第一透镜组与成像面之间,第二透镜组被配置为可沿光轴在第一透镜组与成像面之间移动;第一透镜组的有效焦距FG1、第二透镜组的有效焦距FG2、成像镜头在对焦无穷远时的有效焦距Finf满足:1<(FG1-FG2)/Finf<2。
根据上述成像镜头,通过设置第一透镜组和第二透镜组,并对两个透镜组中的透镜的屈折力进行限定,使成像镜头能够接收更大角度的入射光线,并收敛成像镜头的像差及色差,实现长焦大光圈的特征并提升成像镜头的成像性能。同时,对第一透镜组和第二透镜组的有效焦距与成像镜头对焦无穷远时的有效焦距进行设计,可提高成像镜头在无穷远物距到近焦物距下的成像质量。
在一种实现方式中,第一透镜的物侧面于近光轴处为凸面;第二透镜的物侧面于近光轴处为凹面,第二透镜的像侧面于近光轴处为凹面;第三透镜的物侧面于近光轴处为凸面,第三透镜的像侧面于近光轴处为凸面;第四透镜的物侧面于近光轴处为凹面,第四透镜的像侧面于近光轴处为凸面;第五透镜的像侧面于近光轴处为凹面;第六透镜的物侧面于近光轴处为凹面,第六透镜的像侧面于近光轴处为凹面。这样,通过合理设计第一透镜组和第二透镜组中不同透镜的面型,使成像镜头能够接收更大角度的入射光线,并使进入成像镜头的光线平稳过渡,令光线的走势更加平顺,从而实现大光圈、大靶面的特征,以提高成像镜头的成像质量。
在一种实现方式中,第一透镜的有效焦距f1,与成像镜头在对焦无穷远时的有效焦距Finf满足:0.3<f1/Finf<1。这样,通过对第一透镜的有效焦距进行约束,能够平衡成像镜头的球差,提高成像镜头的成像质量。同时第一透镜还可使成像镜头能够接收更大角度的入射光线,扩大成像镜头的视场角范围,进而实现长焦大光圈、大靶面的特征。
在一种实现方式中,第一透镜的有效焦距f1,与第二透镜的有效焦距f2满足:-2.8<f1/f2<-1.5。这样,通过对第一透镜和第二透镜的有效焦距的约束,使第二透镜能够对经由第一透镜入射的光线进行过渡,减少大角度入射光线的弯折角度,平衡成像镜头的慧差,同时保证整个系统在高低温状态下的成像性能。
在一种实现方式中,成像镜头在对焦无穷远时的有效焦距Finf,与成像镜头在对焦微距时的有效焦距Fmac满足:Finf/Fmac<1.5。这样,通过约束成像镜头在远焦状态和近焦状态的有效焦距的比例,从而对第二透镜组在光轴上的移动范围进行限定,在具有较高成像性能的基础上,实现成像镜头的小型化。
在一种实现方式中,第三透镜的有效焦距f3,与第一透镜组的有效焦距FG1满足:0.2<f3/FG1<1.0。这样,通过约束第三透镜的有效焦距,使第三透镜能够将经由第一透镜和第二透镜入射的光线进行收缩,减少边缘光线的偏差,从而平衡成像镜头的球差及慧差,提高长焦大光圈的成像镜头的成像质量。
在一种实现方式中,第六透镜的有效焦距f6,与第二透镜组的有效焦距FG2满足:0.5<f6/FG2<3。这样,通过约束第六透镜的有效焦距与第二透镜组的有效焦距的比例,可对成像镜头的场曲进行平衡,提高成像镜头近焦状态下的成像性能。
在一种实现方式中,第四透镜在光轴上的中心厚度CT4、第四透镜的物侧面的曲率半径R41,以及,第四透镜的像侧面的曲率半径R42满足:0.5<CT4*(R42/R41)<3。这样,通过对第四透镜的中心厚度及物侧面、像侧面的曲率半径进行约束,可以控制第四透镜的形状,对光线进行有效控制,从而对场曲和像散进行平衡,并有利于实现大靶面的特征,提高成像镜头的成像质量。
在一种实现方式中,第三透镜的像侧面的曲率半径R32,与第四透镜的物侧面的曲率半径R41满足:0.5<R41/R32<5。这样,可对第一透镜组和第二透镜组中相邻的透镜进行约束,使光线平缓地由第一透镜组进入第二透镜组中,减少第一透镜组和第二透镜组间的组装公差敏感性,降低组装难度,提高成像镜头的成像质量及组装工艺性。
在一种实现方式中,第四透镜和第五透镜的组合焦距f45,与第五透镜和第六透镜在光轴上的空间间隔T56满足:-100<f45/T56<-5。这样,通过分配第二透镜组中第四透镜和第五透镜的组合焦距以及第五透镜和第六透镜在光轴上的空间间隔,使第二透镜组能够平衡场曲、像散,同时还可为结构件预留组装位置,便于成像镜头设置在终端设备中。
在一种实现方式中,微距对焦时第六透镜像侧面和成像面在光轴方向的距离BFLmin,与第一透镜物侧面和成像面在光轴方向的距离TTL满足:BFLmin/TTL>0.05。这样,可通过对第六透镜在近焦状态时像侧面和成像面的距离的约束,对成像镜头的对焦行程进行优化,同时还可对成像镜头进行结构优化,便于音圈马达结构的排布,进而实现成像镜头的小型化。
第二方面,本申请实施例提供了一种摄像模组,由物侧至像侧依次包括:光阑、如前述中任一种成像镜头,以及,成像面。根据上述摄像模组,具有该成像镜头的摄像模组在结构小型化的基础上,还具有长焦大光圈、大靶面的特征,从而提高摄像模组的成像性能。
第三方面,本申请实施例提供了一种电子设备,包括前面板、中框、后盖、以及如前述的摄像模组,其中:前面板上设有显示屏,中框设置在前面板与后盖之间,后盖上设有摄像孔;摄像模组通过摄像孔设置在电子设备中,摄像模组中的成像镜头的光轴方向与电子设备的厚度方向平行。由此,可使电子设备中设有该摄像模组,进而通过该摄像模组,实现小型化。
为了更清楚地说明本申请的技术方案,下面将对实施例中所需要使用的附图作简单地介绍,显而易见地,对于本领域普通技术人员而言,在不付出创造性劳动性的前提下,还可以根据这些附图获得其他的附图。
图1为具有电子摄像功能的电子设备在厚度方向上的结构示意图;
图2为摄像模组150的内部结构示意图;
图3为本申请实施例提供的一种摄像模组200的结构示意图;
图4为本申请实施例提供的另一种摄像模组200的结构示意图;
图5为本申请实施例一提供的成像镜头210在对焦无穷远时的结构示意图;
图6为本申请实施例一提供的成像镜头210在对焦微距时的结构示意图;
图7为本申请实施例一提供的成像镜头210在对焦无穷远时的像散曲线图和畸变曲线图;
图8为本申请实施例一提供的成像镜头210在对焦微距时的像散曲线图和畸变曲线图;
图9为本申请实施例二提供的成像镜头210在对焦无穷远时的结构示意图;
图10为本申请实施例二提供的成像镜头210在对焦微距时的结构示意图;
图11为本申请实施例二提供的成像镜头210在对焦无穷远时的像散曲线图和畸变曲线图;
图12为本申请实施例二提供的成像镜头210在对焦微距时的像散曲线图和畸变曲线图;
图13为本申请实施例三提供的成像镜头210在对焦无穷远时的结构示意图;
图14为本申请实施例三提供的成像镜头210在对焦微距时的结构示意图;
图15为本申请实施例三提供的成像镜头210在对焦无穷远时的像散曲线图和畸变曲线图;
图16为本申请实施例三提供的成像镜头210在对焦微距时的像散曲线图和畸变曲线图;
图17为本申请实施例四提供的成像镜头210在对焦无穷远时的结构示意图;
图18为本申请实施例四提供的成像镜头210在对焦微距时的结构示意图;
图19为本申请实施例四提供的成像镜头210在对焦无穷远时的像散曲线图和畸变曲线图;
图20为本申请实施例四提供的成像镜头210在对焦微距时的像散曲线图和畸变曲线图;
图21为本申请实施例五提供的成像镜头210在对焦无穷远时的结构示意图;
图22为本申请实施例五提供的成像镜头210在对焦微距时的结构示意图;
图23为本申请实施例五提供的成像镜头210在对焦无穷远时的像散曲线图和畸变曲线图;
图24为本申请实施例五提供的成像镜头210在对焦微距时的像散曲线图和畸变曲线图;
图25为本申请实施例六提供的成像镜头210在对焦无穷远时的结构示意图;
图26为本申请实施例六提供的成像镜头210在对焦微距时的结构示意图;
图27为本申请实施例六提供的成像镜头210在对焦无穷远时的像散曲线图和畸变曲线图;
图28为本申请实施例六提供的成像镜头210在对焦微距时的像散曲线图和畸变曲线图;
图29为本申请实施例中一种电子设备在厚度方向上的结构示意图;
图30为本申请实施例中一种电子设备的示意图。
下面将结合本申请实施例中的附图,对本申请实施例中的技术方案进行清楚地描述。显然,所描述的实施例是本申请的一部分实施例,而不是全部实施例。基于本申请的实施例,本领域普通技术人员在没有做出创造性劳动的前提下所得到的其他实施例,都属于本申请的保护范围。
以下,术语“第一”、“第二”等仅用于描述目的,而不能理解为指示或暗示相对重要性或者隐含指明所指示的技术特征的数量。由此,限定有“第一”、“第二”等的特征可以明示或者隐含地包括一个或者更多个该特征。在本申请的描述中,除非另有说明,“多个”的含义是两个或两个以上。
此外,本申请中,“上”、“下”等方位术语是相对于附图中的部件示意置放的方位来定义的,应当理解到,这些方向性术语是相对的概念,它们用于相对于的描述和澄清,其可以根据附图中部件所放置的方位的变化而相应地发生变化。
在附图中,为了便于说明,夸大了透镜的厚度和尺寸和比例等参数。因此,附图中所示的球面或者非球面的厚度、尺寸、形状等参数仅作为示意,不代表非球面或者非球面真实形状。也就是说,球面或者非球面的形状不限于附图中示出的球面或非球面的形状。
在本申请实施例中,透镜的中心区域为近轴区域,即光轴附近的区域。透镜的边缘区域则为远轴区域,即透镜中远离光轴的区域。若透镜的表面为凸面且未界定该凸面位置时,表示该透镜的表面至少于中心区域为凸面。若透镜的表面为凹面且未界定该凹面位置时,表示该透镜的表面至少于中心区域为凹面。
本申请的实施方式部分使用的术语仅用于对本申请的具体实施例进行解释,而非旨在限定本申请,下面将结合附图对本申请的实施例进行详细描述。
随着摄像设备技术的发展,越来越多的移动终端设备具备摄像功能,如智能手机、平板电脑、摄像机、数码相机等设备,均设有摄影模块来实现摄影功能。本申请实施例以智能手机为例进行说明。
图1为具有电子摄像功能的电子设备在厚度方向上的结构示意图。如图1所示,该电子设备100包括前面板110、中框120、后盖130、电子元件140和摄像模组150,其中前面板110、中框120和后盖130围合形成一个腔室,电子元件140和摄像模组150设置在该腔室内。
在本申请实施例中,摄像模组150可为电子设备100的前置摄像头和/或后置摄像头,对于摄像模组150的具体设置位置本申请中不做限制。
图2为摄像模组150的内部结构示意图,如图2所示,摄像模组150包括光阑151、成像镜头152和图像传感器(Sensor)153。摄像模组150还可以包括其它与成像相关的组件,例如:保护膜、音圈马达(Voice Coil Motor,VCM)、滤光片、底座、导电布、软硬结合板和连接器等,此处不一一列举。
为了满足用户对电子设备100的摄像功能的要求,需要成像镜头152在远距、微距以及
暗光条件下均具有良好的成像质量,示例性的,可通过组合多个透镜的方式构成成像镜头152并进行成像。如图2所示,成像镜头152包括n个沿成像镜头152的光轴方向依次排列的透镜1521,其中n为大于1的正整数,成像镜头152的光轴方向同电子设备100的厚度方向。
图像传感器153包括感光元件,如电荷耦合元件(Charge coupled Device,CCD)、互补金属氧化物半导体(Complementary Metal Oxide Semiconductor,CMOS)。图像传感器153用于感应成像镜头152聚焦的光线,并在成像面上形成对应于景物的电子图像,其中,成像面是图像传感器153朝向透镜1521的一侧表面。
随着成像镜头152中透镜1521的数量的增加,成像镜头152汇聚光线的能力越高,可以有效提高成像镜头152的解析力和对比度,且能够提高成像镜头152的防眩光效果及成像质量。但是,相应的,成像镜头152的厚度也会越大。
为了便于用户的手持,以及提高电子设备100的美观度,会逐渐降低电子设备100在厚度方向上的尺寸。为了适应电子设备100在厚度方向上缩小的尺寸,摄像模组150在电子设备100的厚度方向上的尺寸也需要缩小,相应的,成像镜头152在电子设备100的厚度方向上的尺寸也需要缩小。
在此基础上,随用户对摄影效果要求的提升,为了实现在远景、微距及暗光场景中均具有良好的摄影效果,需要通过应用长焦镜头的摄像模组150进行成像。但传统的长焦镜头通过马达移动镜头整体来实现对焦,不利于摄像模组150的小型化,且通过马达移动镜头实现对焦,在微距时长焦镜头的成像质量很差,长焦微距拍摄效果较差。同时受限于移动终端中模组体积的要求,小型化后的长焦镜头的光圈较小、靶面较小,暗光拍摄效果差。
为了解决上述问题,需要在保证成像镜头152包括足够数量的透镜1521,以及有效控制成像镜头152在电子设备100的厚度方向上的尺寸的基础上,还需要对成像镜头152中的透镜1521做出合理的设计,从而提高其在微距或暗光环境中的成像质量。
图3为本申请实施例提供的一种摄像模组200的结构示意图,图4为本申请实施例提供的另一种摄像模组200的结构示意图。
在本申请实施例中,如图3所示,摄像模组200沿光轴201从物侧至像侧依次包括光阑ST0、成像镜头210和成像面L8。在一些实施例中,如图4所示,摄像模组200还可以包括滤光片L7,滤光片L7设置于成像镜头210和成像面L8之间。
如图3和图4所示,成像镜头210沿光轴201从物侧至像侧依次包括第一透镜组211和第二透镜组212,其中第一透镜组211沿光轴201从物侧至像侧依次包括第一透镜L1、第二透镜L2和第三透镜L3;第二透镜组212沿光轴201从物侧至像侧依次包括第四透镜L4、第五透镜L5和第六透镜L6。
其中,第一透镜组211的位置相对于摄像模组200的成像面L8固定;第二透镜组212位于第一透镜组211与成像面L8之间,第二透镜组212被配置为可沿光轴201在第一透镜组211与成像面L8之间移动。
应当理解的是,在本申请实施例中,物侧是指靠近所拍摄景物的一侧,像侧是指靠近图像传感器的一侧。因此,成像镜头210中的每个透镜均具有物侧面和像侧面,其中,物侧面是指透镜中朝向物侧的镜面,像侧面是指透镜中朝向像侧的镜面。如图3和图4所示,第一透镜L1包括物侧面E11和像侧面E12,第二透镜L2包括物侧面E21和像侧面E22,第三透镜L3包括物侧面E31和像侧面E32,第四透镜L4包括物侧面E41和像侧面E42,第五透镜L5包括物侧面E51和像侧面E52,第六透镜L6包括物侧面E61和像侧面E62。
如图3和图4所示,光阑ST0设置在物侧与成像镜头210之间,且在部分实施例中,光阑ST0为环形片状结构,能够阻挡由成像镜头210边缘入射的光线。应当理解的是,光阑ST0
的圈口越大,通光量越高,光阑ST0的圈口越小,通光量越低。
在部分实施例中,滤光片L7也具有物侧面IR1和像侧面IR2,滤光片L7用于校正色彩偏差和/或保护位于成像面L8上的感光元件。滤光片L7可以包括蓝玻璃和/或IR-CUT双滤镜等,对于滤光片L7的具体种类本申请实施例中不做限制。
在实际应用中,入射光线在进入成像镜头210前,会有部分边缘光线被光阑ST0拦截,无法进入成像镜头210中。而未被光阑ST0拦截的入射光线则从第一透镜L1的物侧面E11射入,而后入射光线依次经过后续各个透镜,从第六透镜L6的像侧面E62射出。出射光线从滤光片L7的物侧面IR1射入并经由像侧面IR2射出,经过滤光片L7过滤处理的出射光线入射至成像面L8上,由成像面L8感应该光线,并生成对应的电子图像。
在本申请实施例中,为了提高摄像模组200的成像质量,如图3所示,第一透镜L1具有正屈折力,第二透镜L2具有负屈折力,第三透镜L3具有正屈折力,第四透镜L4具有正屈折力,第五透镜L5具有负屈折力,第六透镜L6具有负屈折力。
进一步的,第一透镜L1的物侧面E11于近光轴201处为凸面,第一透镜L1的像侧面E12于近光轴201处可为凸面、也可为凹面;第二透镜L2的物侧面E21于近光轴201处为凹面,第二透镜L2的像侧面E22于近光轴201处为凹面;第三透镜L3的物侧面E31于近光轴201处为凸面,第三透镜L3的像侧面E32于近光轴201处为凸面;第四透镜L4的物侧面E41于近光轴201处为凹面,第四透镜L4的像侧面E42于近光轴201处为凸面;第五透镜L5的物侧面E51于近光轴201处可为凸面、也可为凹面,第五透镜L5的像侧面E52于近光轴201处为凹面;第六透镜L6的物侧面E61于近光轴201处为凹面,第六透镜L6的像侧面E62于近光轴201处为凹面。
需要说明的是,透镜的物侧面的凹凸以像侧为参考,物侧面背离像侧弯曲为凸,物侧面朝向像侧弯曲为凹。透镜的像侧面的凹凸以物侧为参考,像侧面朝向物侧弯曲为凹,像侧面背离物侧弯曲为凸。
配合不同透镜的面型设计,不同的透镜具有不同的光学性能。其中,具有正屈折力的第一透镜L1,能够快速汇聚入射光线,收敛成像镜头210的通光口径,同时还可接收更大角度的入射光线,提高成像的视场角范围。
具有负屈折力的第二透镜L2,则可使大角度的入射光线过渡得更加平缓,减少场曲和球差。
具有正屈折力的第三透镜L3,可以收缩入射光线,减少边缘光线的偏差,从而平衡成像镜头的球差及慧差。
具有正屈折力的第四透镜L4,可以对成像镜头210产生的场曲和像散进行平衡。
具有负屈折力的第五透镜L5,可以减少成像镜头210产生的像差和色差。
具有负屈折力的第六透镜L6,可以平衡像差和场曲,并有利于光线平缓地向成像面过渡。
示例性的,第一透镜组211的有效焦距FG1、第二透镜组212的有效焦距FG2、成像镜头210在对焦无穷远时的有效焦距Finf满足关系式(1):
1<(FG1-FG2)/Finf<2 (1)
1<(FG1-FG2)/Finf<2 (1)
通过对第一透镜组211和第二透镜组212的有效焦距与成像镜头210对焦无穷远时的有效焦距进行设计,可提高成像镜头在无穷远物距到近焦物距下的成像质量,避免对焦不同距离物体时产生的成像质量不一的情况。
在一些实施例中,第一透镜L1的有效焦距f1,与成像镜头210在对焦无穷远时的有效焦距Finf满足关系式(2):
0.3<f1/Finf<1 (2)
0.3<f1/Finf<1 (2)
在本实施例中,通过对第一透镜L1的有效焦距f1进行约束,能够平衡成像镜头210的球差,提高成像镜头210的成像质量。同时结合第一透镜L1的面型设计,第一透镜L1还可使成像镜头210能够接收更大角度的入射光线,扩大成像镜头210的视场角范围,进而实现长焦大光圈、大靶面的特征。
在一些实施例中,第一透镜L1的有效焦距f1,与第二透镜L2的有效焦距f2满足关系式(3):
-2.8<f1/f2<-1.5 (3)
-2.8<f1/f2<-1.5 (3)
这样,通过对第一透镜L1和第二透镜L2的有效焦距的约束,使第二透镜L2能够对经由第一透镜L1入射的光线进行过渡,减少大角度入射光线的弯折角度,平衡成像镜头210的慧差,同时保证整个系统在高低温状态下的成像性能。
在一些实施例中,成像镜头210在对焦无穷远时的有效焦距Finf,与成像镜头210在对焦微距时的有效焦距Fmac满足关系式(4):
Finf/Fmac<1.5 (4)
Finf/Fmac<1.5 (4)
这样,通过约束成像镜头210在远焦状态和近焦状态的有效焦距的比例,从而对第二透镜组212在光轴201上的移动范围进行限定,在具有较高成像性能的基础上,实现成像镜头的小型化,使得成像镜头210可应用在厚度更小的电子设备当中。
在一些实施例中,第三透镜L3的有效焦距f3,与第一透镜组211的有效焦距FG1满足关系式(5):
0.2<f3/FG1<1.0 (5)
0.2<f3/FG1<1.0 (5)
这样,通过约束第三透镜L3的有效焦距,使第三透镜L3能够将经由第一透镜L1和第二透镜L2入射的光线进行收缩,减少边缘光线的偏差,从而平衡成像镜头210的球差及慧差,提高长焦大光圈的成像镜头210的成像质量。
在一些实施例中,第六透镜L6的有效焦距f6,与第二透镜组212的有效焦距FG2满足关系式(6):
0.5<f6/FG2<3 (6)
0.5<f6/FG2<3 (6)
这样,通过约束第六透镜L6的有效焦距与第二透镜组212的有效焦距的比例,可对成像镜头210的场曲进行平衡,提高成像镜头210近焦状态下的成像性能。
在一些实施例中,第四透镜L4在光轴201上的中心厚度CT4、第四透镜L4的物侧面E41的曲率半径R41,以及,第四透镜L4的像侧面E42的曲率半径R42满足关系式(7):
0.5<CT4*(R42/R41)<3 (7)
0.5<CT4*(R42/R41)<3 (7)
这样,通过对第四透镜L4的中心厚度及物侧面E41、像侧面E42的曲率半径进行约束,可以控制第四透镜L4的形状,对光线进行有效控制,从而对场曲和像散进行平衡,并有利于实现大靶面的特征,提高成像镜头210的成像质量。
在一些实施例中,第三透镜L3的像侧面E32的曲率半径R32,与第四透镜L4的物侧面E41的曲率半径R41满足关系式(8):
0.5<R41/R32<5 (8)
0.5<R41/R32<5 (8)
这样,可对第一透镜组211和第二透镜组212中相邻的透镜进行约束,使光线平缓地由第一透镜组211进入第二透镜组212中,减少第一透镜组211和第二透镜组212间的组装公差敏感性,降低组装难度,提高成像镜头210的成像质量及组装工艺性。
在一些实施例中,第四透镜L4和第五透镜L5的组合焦距f45,与第五透镜L5和第六透镜L6在光轴201上的空间间隔T56满足关系式(9):
-100<f45/T56<-5 (9)
-100<f45/T56<-5 (9)
这样,通过分配第二透镜组212中第四透镜L4和第五透镜L5的组合焦距以及第五透镜L5和第六透镜L6在光轴201上的空间间隔,使第二透镜组212能够平衡场曲、像散,同时还可为结构件预留组装位置,便于成像镜头210设置在终端设备中。
在一些实施例中,微距对焦时第六透镜L6的像侧面E62和成像面L8在光轴201方向的距离BFLmin,与第一透镜L1的物侧面E11和成像面L8在光轴201方向的距离TTL满足关系式(10):
BFLmin/TTL>0.05 (10)
BFLmin/TTL>0.05 (10)
这样,可通过对第六透镜L6在近焦状态时像侧面E62和成像面L8的距离的约束,对成像镜头210的对焦行程进行优化,同时还可对成像镜头210进行结构优化,便于音圈马达结构的排布,进而实现成像镜头210的小型化。
在一些实施例中,各透镜包括至少一个非球面透镜,即第一透镜L1的物侧面E11至第六透镜L6的像侧面E62中至少一个镜面为非球面镜面。非球面透镜具有从透镜中心到透镜边缘,曲率连续变化的特点。与从透镜中心到透镜边缘具有恒定曲率的球面透镜不同,非球面透镜具有更佳的曲率半径特性,具有改善像差的优点。采用非球面透镜后,能够尽可能地消除在成像的时候出现的像差,从而提高成像质量。
在一些实施例中,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和第六透镜L6中每个透镜的物侧面和像侧面中至少一个为非球面镜面。
在一些实施例中,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和第六透镜L6中每个透镜的物侧面和像侧面均为非球面镜面。
在一些实施例中,各透镜包括至少一个玻璃透镜。示例性的,成像镜头210中的第一透镜L1可为玻璃透镜,其余可为塑料透镜,相较于塑料透镜来说,玻璃透镜在有更高的折射率的基础上具有较低的色散系数,使第一透镜L1在具有良好的光学性能的条件下,还能够降低其温度敏感性,使成像镜头210能够应用在更多的环境中。前述透镜材质仅为本申请中一种示例性说明,本申请中对于各透镜的具体材质构成不做限制。
由此,本申请实施例提供的成像镜头210既可以在暗环境下提高镜头的进光量,增强画质,又可以避免在亮环境下出现过度曝光等不利影响。通过合理分配成像镜头中各透镜的屈折力、面型、材质、尺寸等,可以有效地汇聚入射光线,降低像差和像散,以在使成像镜头210可以适应终端设备在厚度方向上的尺寸的基础上,有效提高成像镜头210在复杂光环境下的成像质量,并且可以有效提高各透镜的加工及组装的便利性。相应的,本申请实施例提供的摄像模组200也可以在适应终端设备在厚度方向上的尺寸的基础上,具有长焦大光圈、大靶面和高成像质量等特性。
以下将结合具体参数对成像镜头210的部分可选择的实施例进行详细说明。
实施例一
图5为本申请实施例一提供的成像镜头210在对焦无穷远时的结构示意图,图6为本申请实施例一提供的成像镜头210在对焦微距时的结构示意图。如图5和图6所示,摄像模组200沿光轴201由物侧至像侧依次包括:光阑ST0、第一透镜组211、第二透镜组212、滤光片L7和成像面L8。且第一透镜组211沿光轴201由物侧至像侧依次包括第一透镜L1、第二透镜L2和第三透镜L3,第二透镜组212沿光轴201由物侧至像侧依次包括第四透镜L4、第五透镜L5和第六透镜L6。
其中,第一透镜L1具有正屈折力,第一透镜L1的物侧面E11于近光轴201处为凸面,第一透镜L1的像侧面E12于近光轴201处为凹面。第二透镜L2具有负屈折力,第二透镜L2的物侧面E21于近光轴201处为凹面,第二透镜L2的像侧面E22于近光轴201处为凹面。
第三透镜L3具有正屈折力,第三透镜L3的物侧面E31于近光轴201处为凸面,第三透镜L3的像侧面E32于近光轴201处为凸面。第四透镜L4具有正屈折力,第四透镜L4的物侧面E41于近光轴201处为凹面,第四透镜L4的像侧面E42于近光轴201处为凸面。第五透镜L5具有负屈折力,第五透镜L5的物侧面E51于近光轴201处为凸面,第五透镜L5的像侧面E52于近光轴201处为凹面。第六透镜L6具有负屈折力,第六透镜L6的物侧面E61于近光轴201处为凹面,第六透镜L6的像侧面E62于近光轴201处为凹面。
表1示出了实施例一的摄像模组200的基本参数,其中,曲率半径、厚度和焦距的单位均为毫米(mm)。
表1
需要说明的是,表1中列出的厚度数值中,对应于透镜及滤光片物侧面的数值为该透镜或滤光片的中心厚度,即该透镜或滤光片在光轴201上的厚度;而对应于透镜及滤光片像侧面的数值则为该透镜或滤光片与后方部件的物侧面在光轴201上的空间间隔。
如表1所示,成像镜头210在对焦无穷远时,第三透镜L3的像侧面E32与第四透镜L4的物侧面E41之间的空间距离T34=0.56mm,第六透镜L6的像侧面E62与滤光片L7的物侧面IR1之间的空间距离T67=3.83mm。成像镜头210在对焦微距时,第三透镜L3的像侧面E32与第四透镜L4的物侧面E41之间的空间距离T34=3.24mm,第六透镜L6的像侧面E62与滤光片L7的物侧面IR1之间的空间距离T67=1.15mm。
在实施例一中,成像镜头210在对焦无穷远时的有效焦距Finf=18.6mm,成像镜头210在对焦微距时的有效焦距Fmac=13.95mm。成像镜头210对焦无穷远时的F数FNOinf=1.93,成像镜头210对焦微距时的F数FNOmac=1.48。成像镜头210对焦无穷远时的视场角FOVinf=17.22°,成像镜头210对焦微距时的视场角FOVmac=18.08°,第一透镜组211的有效焦距FG1=12.31mm,第二透镜组212的有效焦距FG2=-12.14mm。
需要说明的是,在本实施例中,成像镜头210对焦微距时,镜头距离物面的距离小于或等于12cm。
在本实施例中,由第一透镜L1至第六透镜L6中任一个透镜的物侧面和像侧面均为非球面,各非球面透镜的面型满足(不限于)如下公式(11):
其中,x为非球面沿光轴201方向在高度为h的位置时,距非球面顶点的距离矢高,c为非球面的近轴曲率,c=1/R(近轴曲率c为表1中曲率半径R的倒数),k为圆锥系数,Ai是非球面第i阶的修正系数。下表2-1和表2-2给出了可用于实施例一中各非球面镜面的高次项系数A4、A6、A8、A10、A12、A14、A16、A18和A20。
表2-1
表2-2
入射光线经过如图5和图6所示的光阑ST0的拦截,保留部分光线从第一透镜L1的物侧面E11射入,入射光线依次经过各个透镜,从第六透镜L6的像侧面E62射出。出射光线从滤光片L7的物侧面IR1射入并经由像侧面IR2射出,经过滤光片L7过滤处理的出射光线入射在成像面L8上,由成像面L8感应入射光线,并生成对应的电子图像。
图7为本申请实施例一提供的成像镜头210在对焦无穷远时的像散曲线图和畸变曲线图。图8为本申请实施例一提供的成像镜头210在对焦微距时的像散曲线图和畸变曲线图。
其中,像散曲线图用于表示子午像面弯曲和弧矢像面弯曲,畸变曲线图用于表示不同像高对应的畸变大小值,在实施例一中,用于测试参考光线波长为546nm。根据图7和图8可
知,在该参考波长下,实施例一所给出的成像镜头210能够对像散和畸变进行良好的补偿和校正,从而使成像镜头210能够实现良好的成像质量。
实施例二
图9为本申请实施例二提供的成像镜头210在对焦无穷远时的结构示意图,图10为本申请实施例二提供的成像镜头210在对焦微距时的结构示意图。如图9和图10所示,摄像模组200沿光轴201由物侧至像侧依次包括:光阑ST0、第一透镜组211、第二透镜组212、滤光片L7和成像面L8。且第一透镜组211沿光轴201由物侧至像侧依次包括第一透镜L1、第二透镜L2和第三透镜L3,第二透镜组212沿光轴201由物侧至像侧依次包括第四透镜L4、第五透镜L5和第六透镜L6。
其中,第一透镜L1具有正屈折力,第一透镜L1的物侧面E11于近光轴201处为凸面,第一透镜L1的像侧面E12于近光轴201处为凹面。第二透镜L2具有负屈折力,第二透镜L2的物侧面E21于近光轴201处为凹面,第二透镜L2的像侧面E22于近光轴201处为凹面。第三透镜L3具有正屈折力,第三透镜L3的物侧面E31于近光轴201处为凸面,第三透镜L3的像侧面E32于近光轴201处为凸面。第四透镜L4具有正屈折力,第四透镜L4的物侧面E41于近光轴201处为凹面,第四透镜L4的像侧面E42于近光轴201处为凸面。第五透镜L5具有负屈折力,第五透镜L5的物侧面E51于近光轴201处为凸面,第五透镜L5的像侧面E52于近光轴201处为凹面。第六透镜L6具有负屈折力,第六透镜L6的物侧面E61于近光轴201处为凹面,第六透镜L6的像侧面E62于近光轴201处为凹面。
表3示出了实施例二的摄像模组200的基本参数,其中,曲率半径、厚度和焦距的单位均为毫米(mm)。
表3
需要说明的是,表3中列出的厚度数值中,对应于透镜及滤光片物侧面的数值为该透镜
或滤光片的中心厚度,即该透镜或滤光片在光轴201上的厚度;而对应于透镜及滤光片像侧面的数值则为该透镜或滤光片与后方部件的物侧面在光轴201上的空间间隔。
如表3所示,成像镜头210在对焦无穷远时,第三透镜L3的像侧面E32与第四透镜L4的物侧面E41之间的空间距离T34=0.6mm,第六透镜L6的像侧面E62与滤光片L7的物侧面IR1之间的空间距离T67=3.93mm。成像镜头210在对焦微距时,第三透镜L3的像侧面E32与第四透镜L4的物侧面E41之间的空间距离T34=3.48mm,第六透镜L6的像侧面E62与滤光片L7的物侧面IR1之间的空间距离T67=1.05mm。
在实施例二中,成像镜头210在对焦无穷远时的有效焦距Finf=19.95mm,成像镜头210在对焦微距时的有效焦距Fmac=15.10mm。成像镜头210对焦无穷远时的F数FNOinf=1.96,成像镜头210对焦微距时的F数FNOmac=1.52。成像镜头210对焦无穷远时的视场角FOVinf=17.2°,成像镜头210对焦微距时的视场角FOVmac=18.05°,第一透镜组211的有效焦距FG1=13.66mm,第二透镜组212的有效焦距FG2=-12.65mm。
需要说明的是,在本实施例中,成像镜头210对焦微距时,镜头距离物面的距离小于或等于13cm。
在实施例二中,第一透镜L1至第六透镜L6中任意一个透镜的物侧面和像侧面均为非球面,各非球面透镜的面型满足实施例一中的公式(11),表4-1和表4-2示出了可用于实施例二中各非球面镜面的高次项系数。
表4-1
表4-2
入射光线经过如图9和图10所示的光阑ST0的拦截,保留部分光线从第一透镜L1的物
侧面E11射入,入射光线依次经过各个透镜,从第六透镜L6的像侧面E62射出。出射光线从滤光片L7的物侧面IR1射入并经由像侧面IR2射出,经过滤光片L7过滤处理的出射光线入射在成像面L8上,由成像面L8感应入射光线,并生成对应的电子图像。
图11为本申请实施例二提供的成像镜头210在对焦无穷远时的像散曲线图和畸变曲线图。图12为本申请实施例二提供的成像镜头210在对焦微距时的像散曲线图和畸变曲线图。
其中,像散曲线图用于表示子午像面弯曲和弧矢像面弯曲,畸变曲线图用于表示不同像高对应的畸变大小值,在实施例二中,用于测试参考光线波长为555nm。根据图11和图12可知,在该参考波长下,实施例二所给出的成像镜头210能够对像散和畸变进行良好的补偿和校正,从而使成像镜头210能够实现良好的成像质量。
实施例三
图13为本申请实施例三提供的成像镜头210在对焦无穷远时的结构示意图,图14为本申请实施例三提供的成像镜头210在对焦微距时的结构示意图。如图13和图14所示,摄像模组200沿光轴201由物侧至像侧依次包括:光阑ST0、第一透镜组211、第二透镜组212、滤光片L7和成像面L8。且第一透镜组211沿光轴201由物侧至像侧依次包括第一透镜L1、第二透镜L2和第三透镜L3,第二透镜组212沿光轴201由物侧至像侧依次包括第四透镜L4、第五透镜L5和第六透镜L6。
其中,第一透镜L1具有正屈折力,第一透镜L1的物侧面E11于近光轴201处为凸面,第一透镜L1的像侧面E12于近光轴201处为凹面。第二透镜L2具有负屈折力,第二透镜L2的物侧面E21于近光轴201处为凹面,第二透镜L2的像侧面E22于近光轴201处为凹面。第三透镜L3具有正屈折力,第三透镜L3的物侧面E31于近光轴201处为凸面,第三透镜L3的像侧面E32于近光轴201处为凸面。第四透镜L4具有正屈折力,第四透镜L4的物侧面E41于近光轴201处为凹面,第四透镜L4的像侧面E42于近光轴201处为凸面。第五透镜L5具有负屈折力,第五透镜L5的物侧面E51于近光轴201处为凸面,第五透镜L5的像侧面E52于近光轴201处为凹面。第六透镜L6具有负屈折力,第六透镜L6的物侧面E61于近光轴201处为凹面,第六透镜L6的像侧面E62于近光轴201处为凹面。
表5示出了实施例三的摄像模组200的基本参数,其中,曲率半径、厚度和焦距的单位均为毫米(mm)。
表5
需要说明的是,表5中列出的厚度数值中,对应于透镜及滤光片物侧面的数值为该透镜或滤光片的中心厚度,即该透镜或滤光片在光轴201上的厚度;而对应于透镜及滤光片像侧面的数值则为该透镜或滤光片与后方部件的物侧面在光轴201上的空间间隔。
如表5所示,成像镜头210在对焦无穷远时,第三透镜L3的像侧面E32与第四透镜L4的物侧面E41之间的空间距离T34=0.6mm,第六透镜L6的像侧面E62与滤光片L7的物侧面IR1之间的空间距离T67=4.04mm。成像镜头210在对焦微距时,第三透镜L3的像侧面E32与第四透镜L4的物侧面E41之间的空间距离T34=3.47mm,第六透镜L6的像侧面E62与滤光片L7的物侧面IR1之间的空间距离T67=1.17mm。
在实施例三中,成像镜头210在对焦无穷远时的有效焦距Finf=19.98mm,成像镜头210在对焦微距时的有效焦距Fmac=15.03mm。成像镜头210对焦无穷远时的F数FNOinf=1.93,成像镜头210对焦微距时的F数FNOmac=1.48。成像镜头210对焦无穷远时的视场角FOVinf=17.18°,成像镜头210对焦微距时的视场角FOVmac=17.99°,第一透镜组211的有效焦距FG1=13.40mm,第二透镜组212的有效焦距FG2=-13.14mm。
需要说明的是,在本实施例中,成像镜头210对焦微距时,镜头距离物面的距离小于或等于13cm。
在实施例三中,第一透镜L1至第六透镜L6中任意一个透镜的物侧面和像侧面均为非球面,各非球面透镜的面型满足实施例一中的公式(11),表6-1和表6-2示出了可用于实施例三中各非球面镜面的高次项系数。
表6-1
表6-2
入射光线经过如图13和图14所示的光阑ST0的拦截,保留部分光线从第一透镜L1的物侧面E11射入,入射光线依次经过各个透镜,从第六透镜L6的像侧面E62射出。出射光线从滤光片L7的物侧面IR1射入并经由像侧面IR2射出,经过滤光片L7过滤处理的出射光线入射在成像面L8上,由成像面L8感应入射光线,并生成对应的电子图像。
图15为本申请实施例三提供的成像镜头210在对焦无穷远时的像散曲线图和畸变曲线图。图16为本申请实施例三提供的成像镜头210在对焦微距时的像散曲线图和畸变曲线图。
其中,像散曲线图用于表示子午像面弯曲和弧矢像面弯曲,畸变曲线图用于表示不同像高对应的畸变大小值,在实施例三中,用于测试参考光线波长为555nm。根据图15和图16可知,在该参考波长下,实施例三所给出的成像镜头210能够对像散和畸变进行良好的补偿和校正,从而使成像镜头210能够实现良好的成像质量。
实施例四
图17为本申请实施例四提供的成像镜头210在对焦无穷远时的结构示意图,图18为本申请实施例四提供的成像镜头210在对焦微距时的结构示意图。如图17和图18所示,摄像模组200沿光轴201由物侧至像侧依次包括:光阑ST0、第一透镜组211、第二透镜组212、滤光片L7和成像面L8。且第一透镜组211沿光轴201由物侧至像侧依次包括第一透镜L1、第二透镜L2和第三透镜L3,第二透镜组212沿光轴201由物侧至像侧依次包括第四透镜L4、第五透镜L5和第六透镜L6。
其中,第一透镜L1具有正屈折力,第一透镜L1的物侧面E11于近光轴201处为凸面,第一透镜L1的像侧面E12于近光轴201处为凸面。第二透镜L2具有负屈折力,第二透镜L2的物侧面E21于近光轴201处为凹面,第二透镜L2的像侧面E22于近光轴201处为凹面。第三透镜L3具有正屈折力,第三透镜L3的物侧面E31于近光轴201处为凸面,第三透镜L3的像侧面E32于近光轴201处为凸面。第四透镜L4具有正屈折力,第四透镜L4的物侧面E41于近光轴201处为凹面,第四透镜L4的像侧面E42于近光轴201处为凸面。第五透镜L5具有负屈折力,第五透镜L5的物侧面E51于近光轴201处为凹面,第五透镜L5的像侧面E52于近光轴201处为凹面。第六透镜L6具有负屈折力,第六透镜L6的物侧面E61于近光轴201处为凹面,第六透镜L6的像侧面E62于近光轴201处为凹面。
表7示出了实施例四的摄像模组200的基本参数,其中,曲率半径、厚度和焦距的单位均为毫米(mm)。
表7
需要说明的是,表7中列出的厚度数值中,对应于透镜及滤光片物侧面的数值为该透镜或滤光片的中心厚度,即该透镜或滤光片在光轴201上的厚度;而对应于透镜及滤光片像侧面的数值则为该透镜或滤光片与后方部件的物侧面在光轴201上的空间间隔。
如表7所示,成像镜头210在对焦无穷远时,第三透镜L3的像侧面E32与第四透镜L4的物侧面E41之间的空间距离T34=0.6mm,第六透镜L6的像侧面E62与滤光片L7的物侧面IR1之间的空间距离T67=3.88mm。成像镜头210在对焦微距时,第三透镜L3的像侧面E32与第四透镜L4的物侧面E41之间的空间距离T34=3.29mm,第六透镜L6的像侧面E62与滤光片L7的物侧面IR1之间的空间距离T67=1.19mm。
在实施例四中,成像镜头210在对焦无穷远时的有效焦距Finf=18.6mm,成像镜头210在对焦微距时的有效焦距Fmac=13.67mm。成像镜头210对焦无穷远时的F数FNOinf=1.90,成像镜头210对焦微距时的F数FNOmac=1.50。成像镜头210对焦无穷远时的视场角FOVinf=17.19°,成像镜头210对焦微距时的视场角FOVmac=18.16°,第一透镜组211的有效焦距FG1=12.25mm,第二透镜组212的有效焦距FG2=-11.33mm。
需要说明的是,在本实施例中,成像镜头210对焦微距时,镜头距离物面的距离小于或等于12cm。
在实施例四中,第一透镜L1至第六透镜L6中任意一个透镜的物侧面和像侧面均为非球面,各非球面透镜的面型满足实施例一中的公式(11),表8-1和表8-2示出了可用于实施例四中各非球面镜面的高次项系数。
表8-1
表8-2
入射光线经过如图17和图18所示的光阑ST0的拦截,保留部分光线从第一透镜L1的物侧面E11射入,入射光线依次经过各个透镜,从第六透镜L6的像侧面E62射出。出射光线从滤光片L7的物侧面IR1射入并经由像侧面IR2射出,经过滤光片L7过滤处理的出射光线入射在成像面L8上,由成像面L8感应入射光线,并生成对应的电子图像。
图19为本申请实施例四提供的成像镜头210在对焦无穷远时的像散曲线图和畸变曲线图。图20为本申请实施例四提供的成像镜头210在对焦微距时的像散曲线图和畸变曲线图。
其中,像散曲线图用于表示子午像面弯曲和弧矢像面弯曲,畸变曲线图用于表示不同像高对应的畸变大小值,在实施例四中,用于测试参考光线波长为555nm。根据图19和图20可知,在该参考波长下,实施例四所给出的成像镜头210能够对像散和畸变进行良好的补偿和校正,从而使成像镜头210能够实现良好的成像质量。
实施例五
图21为本申请实施例五提供的成像镜头210在对焦无穷远时的结构示意图,图22为本申请实施例五提供的成像镜头210在对焦微距时的结构示意图。如图21和图22所示,摄像模组200沿光轴201由物侧至像侧依次包括:光阑ST0、第一透镜组211、第二透镜组212、滤光片L7和成像面L8。且第一透镜组211沿光轴201由物侧至像侧依次包括第一透镜L1、第二透镜L2和第三透镜L3,第二透镜组212沿光轴201由物侧至像侧依次包括第四透镜L4、第五透镜L5和第六透镜L6。
其中,第一透镜L1具有正屈折力,第一透镜L1的物侧面E11于近光轴201处为凸面,第一透镜L1的像侧面E12于近光轴201处为凸面。第二透镜L2具有负屈折力,第二透镜L2的物侧面E21于近光轴201处为凹面,第二透镜L2的像侧面E22于近光轴201处为凹面。第三透镜L3具有正屈折力,第三透镜L3的物侧面E31于近光轴201处为凸面,第三透镜L3的像侧面E32于近光轴201处为凸面。第四透镜L4具有正屈折力,第四透镜L4的物侧面E41于近光轴201处为凹面,第四透镜L4的像侧面E42于近光轴201处为凸面。第五透镜L5具有负屈折力,第五透镜L5的物侧面E51于近光轴201处为凹面,第五透镜L5的像侧面E52于近光轴201处为凹面。第六透镜L6具有负屈折力,第六透镜L6的物侧面E61于近光轴201处为凹面,第六透镜L6的像侧面E62于近光轴201处为凹面。
表9示出了实施例五的摄像模组200的基本参数,其中,曲率半径、厚度和焦距的单位均为毫米(mm)。
表9
需要说明的是,表9中列出的厚度数值中,对应于透镜及滤光片物侧面的数值为该透镜或滤光片的中心厚度,即该透镜或滤光片在光轴201上的厚度;而对应于透镜及滤光片像侧面的数值则为该透镜或滤光片与后方部件的物侧面在光轴201上的空间间隔。
如表9所示,成像镜头210在对焦无穷远时,第三透镜L3的像侧面E32与第四透镜L4的物侧面E41之间的空间距离T34=0.55mm,第六透镜L6的像侧面E62与滤光片L7的物侧面IR1之间的空间距离T67=3.65mm。成像镜头210在对焦微距时,第三透镜L3的像侧面E32与第四透镜L4的物侧面E41之间的空间距离T34=2.83mm,第六透镜L6的像侧面E62与滤光片L7的物侧面IR1之间的空间距离T67=1.37mm。
在实施例五中,成像镜头210在对焦无穷远时的有效焦距Finf=18.55mm,成像镜头210在对焦微距时的有效焦距Fmac=14.15mm。成像镜头210对焦无穷远时的F数FNOinf=1.88,成像镜头210对焦微距时的F数FNOmac=1.47。成像镜头210对焦无穷远时的视场角FOVinf=17.22°,成像镜头210对焦微距时的视场角FOVmac=17.86°,第一透镜组211的有效焦距FG1=12.08,第二透镜组212的有效焦距FG2=-11.24。
需要说明的是,在本实施例中,成像镜头210对焦微距时,镜头距离物面的距离小于或等于13cm。
在实施例五中,第一透镜L1至第六透镜L6中任意一个透镜的物侧面和像侧面均为非球面,各非球面透镜的面型满足实施例一中的公式(11),表10-1和表10-2示出了可用于实施例五中各非球面镜面的高次项系数。
表10-1
表10-2
入射光线经过如图21和图22所示的光阑ST0的拦截,保留部分光线从第一透镜L1的物侧面E11射入,入射光线依次经过各个透镜,从第六透镜L6的像侧面E62射出。出射光线从滤光片L7的物侧面IR1射入并经由像侧面IR2射出,经过滤光片L7过滤处理的出射光线入射在成像面L8上,由成像面L8感应入射光线,并生成对应的电子图像。
图23为本申请实施例五提供的成像镜头210在对焦无穷远时的像散曲线图和畸变曲线图。图24为本申请实施例五提供的成像镜头210在对焦微距时的像散曲线图和畸变曲线图。
其中,像散曲线图用于表示子午像面弯曲和弧矢像面弯曲,畸变曲线图用于表示不同像高对应的畸变大小值,在实施例五中,用于测试参考光线波长为555nm。根据图23和图24可知,在该参考波长下,实施例五所给出的成像镜头210能够对像散和畸变进行良好的补偿和校正,从而使成像镜头210能够实现良好的成像质量。
实施例六
图25为本申请实施例六提供的成像镜头210在对焦无穷远时的结构示意图,图26为本申请实施例六提供的成像镜头210在对焦微距时的结构示意图。如图25和图26所示,摄像模组200沿光轴201由物侧至像侧依次包括:光阑ST0、第一透镜组211、第二透镜组212、滤光片L7和成像面L8。且第一透镜组211沿光轴201由物侧至像侧依次包括第一透镜L1、第二透镜L2和第三透镜L3,第二透镜组212沿光轴201由物侧至像侧依次包括第四透镜L4、第五透镜L5和第六透镜L6。
其中,第一透镜L1具有正屈折力,第一透镜L1的物侧面E11于近光轴201处为凸面,第一透镜L1的像侧面E12于近光轴201处为凹面。第二透镜L2具有负屈折力,第二透镜L2的物侧面E21于近光轴201处为凹面,第二透镜L2的像侧面E22于近光轴201处为凹面。第三透镜L3具有正屈折力,第三透镜L3的物侧面E31于近光轴201处为凸面,第三透镜L3的像侧面E32于近光轴201处为凸面。第四透镜L4具有正屈折力,第四透镜L4的物侧
面E41于近光轴201处为凹面,第四透镜L4的像侧面E42于近光轴201处为凸面。第五透镜L5具有负屈折力,第五透镜L5的物侧面E51于近光轴201处为凸面,第五透镜L5的像侧面E52于近光轴201处为凹面。第六透镜L6具有负屈折力,第六透镜L6的物侧面E61于近光轴201处为凹面,第六透镜L6的像侧面E62于近光轴201处为凹面。
表11示出了实施例六的摄像模组200的基本参数,其中,曲率半径、厚度和焦距的单位均为毫米(mm)。
表11
需要说明的是,表11中列出的厚度数值中,对应于透镜及滤光片物侧面的数值为该透镜或滤光片的中心厚度,即该透镜或滤光片在光轴上的厚度;而对应于透镜及滤光片像侧面的数值则为该透镜或滤光片与后方部件的物侧面在光轴201上的空间间隔。
如表11所示,成像镜头210在对焦无穷远时,第三透镜L3的像侧面E32与第四透镜L4的物侧面E41之间的空间距离T34=0.56mm,第六透镜L6的像侧面E62与滤光片L7的物侧面IR1之间的空间距离T67=3.93mm。成像镜头210在对焦微距时,第三透镜L3的像侧面E32与第四透镜L4的物侧面E41之间的空间距离T34=3.28mm,第六透镜L6的像侧面E62与滤光片L7的物侧面IR1之间的空间距离T67=1.21mm。
在实施例六中,成像镜头210在对焦无穷远时的有效焦距Finf=18.6mm,成像镜头210在对焦微距时的有效焦距Fmac=13.96mm。成像镜头210对焦无穷远时的F数FNOinf=1.92,成像镜头210对焦微距时的F数FNOmac=1.47。成像镜头210对焦无穷远时的视场角FOVinf=17.21°,成像镜头210对焦微距时的视场角FOVmac=18.1°,第一透镜组211的有效焦距FG1=12.34mm,第二透镜组212的有效焦距FG2=-12.32mm。
需要说明的是,在本实施例中,成像镜头210对焦微距时,镜头距离物面的距离小于或等于13cm。
在实施例六中,第一透镜L1至第六透镜L6中任意一个透镜的物侧面和像侧面均为非球面,各非球面透镜的面型满足实施例一中的公式(11),表12-1和表12-2示出了可用于实施例六中各非球面镜面的高次项系数。
表12-1
表12-2
入射光线经过如图25和图26所示的光阑ST0的拦截,保留部分光线从第一透镜L1的物侧面E11射入,入射光线依次经过各个透镜,从第六透镜L6的像侧面E62射出。出射光线从滤光片L7的物侧面IR1射入并经由像侧面IR2射出,经过滤光片L7过滤处理的出射光线入射在成像面L8上,由成像面L8感应入射光线,并生成对应的电子图像。
图27为本申请实施例六提供的成像镜头210在对焦无穷远时的像散曲线图和畸变曲线图。图28为本申请实施例六提供的成像镜头210在对焦微距时的像散曲线图和畸变曲线图。
其中,像散曲线图用于表示子午像面弯曲和弧矢像面弯曲,畸变曲线图用于表示不同像高对应的畸变大小值,在实施例六中,用于测试参考光线波长为546nm。根据图27和图28可知,在该参考波长下,实施例六所给出的成像镜头210能够对像散和畸变进行良好的补偿和校正,从而使成像镜头210能够实现良好的成像质量。
综上,在前述实施例一至实施例六中给出了成像镜头210的参数设计的基础上,参见表13,实施例一至实施例六分别满足前述关系式(1)至关系式(10)。
表13
图29为本申请实施例中一种电子设备在厚度方向上的结构示意图;图30为本申请实施例中一种电子设备的示意图。
本申请在提供前述成像镜头和摄像模组的基础上,本申请还提供一种电子设备,如图29和图30所示,该电子设备中包括前面板310、中框320、后盖330以及包含前述任一种成像镜头的摄像模组200,其中前面板310上设有显示屏311,中框320设置在前面板310和后盖330之间,且后盖330上设有摄像孔331,摄像模组200通过摄像孔331设置在该电子设备中,且摄像模组200中的成像镜头的光轴201方向与该电子设备的厚度方向平行。
在本申请实施例中,前面板310、中框320和后盖330围合形成的腔室中还包括电子元件340,电子元件340包括且不限于处理器、天线、传感器、陀螺仪、扬声器等器件,以使该电子设备能够通过显示屏311显示由摄像模组200得到图像或视频。
应当理解的是,通过后盖330上的摄像孔331设置在电子设备中的摄像模组200,能够作为该电子设备的后置摄像头,来接收位于后盖330远离前面板310一侧的入射光线,以生成相应的电子图像。
在部分实施例中,摄像模组200还可作为该电子设备的前置摄像头。示例性的,可在该电子设备的前面板310上设置摄像孔,并将摄像模组200通过前面板310上的摄像孔进行安装,从而接收位于前面板310远离后盖330一侧的入射光线,以生成相应的电子图像。
以上的具体实施方式,对本发明的目的、技术方案和有益效果进行了进一步详细说明,所应理解的是,以上仅为本发明的具体实施方式而已,并不用于限定本发明的保护范围,凡在本发明的技术方案的基础之上,所做的任何修改、等同替换、改进等,均应包括在本发明的保护范围之内。
Claims (13)
- 一种成像镜头,其特征在于,沿光轴从物侧至像侧依次包括第一透镜组和第二透镜组;所述第一透镜组沿所述光轴从物侧至像侧依次包括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;所述第二透镜组沿所述光轴从物侧至像侧依次包括具有正屈折力的第四透镜、具有负屈折力的第五透镜、具有负屈折力的第六透镜;其中,所述第一透镜组的位置相对于摄像模组的成像面固定;所述第二透镜组位于所述第一透镜组与所述成像面之间,所述第二透镜组被配置为可沿所述光轴在所述第一透镜组与所述成像面之间移动;所述第一透镜组的有效焦距FG1、所述第二透镜组的有效焦距FG2、所述成像镜头在对焦无穷远时的有效焦距Finf满足:1<(FG1-FG2)/Finf<2。
- 根据权利要求1所述的成像镜头,其特征在于,所述第一透镜的物侧面于近光轴处为凸面;所述第二透镜的物侧面于近光轴处为凹面,所述第二透镜的像侧面于近光轴处为凹面;所述第三透镜的物侧面于近光轴处为凸面,所述第三透镜的像侧面于近光轴处为凸面;所述第四透镜的物侧面于近光轴处为凹面,所述第四透镜的像侧面于近光轴处为凸面;所述第五透镜的像侧面于近光轴处为凹面;所述第六透镜的物侧面于近光轴处为凹面,所述第六透镜的像侧面于近光轴处为凹面。
- 根据权利要求1所述的成像镜头,其特征在于,所述第一透镜的有效焦距f1,与所述成像镜头在对焦无穷远时的有效焦距Finf满足:0.3<f1/Finf<1。
- 根据权利要求1所述的成像镜头,其特征在于,所述第一透镜的有效焦距f1,与所述第二透镜的有效焦距f2满足:-2.8<f1/f2<-1.5。
- 根据权利要求1所述的成像镜头,其特征在于,所述成像镜头在对焦无穷远时的有效焦距Finf,与所述成像镜头在对焦微距时的有效焦距Fmac满足:Finf/Fmac<1.5。
- 根据权利要求1所述的成像镜头,其特征在于,所述第三透镜的有效焦距f3,与所述第一透镜组的有效焦距FG1满足:0.2<f3/FG1<1.0。
- 根据权利要求1所述的成像镜头,其特征在于,所述第六透镜的有效焦距f6,与所述第二透镜组的有效焦距FG2满足:0.5<f6/FG2<3。
- 根据权利要求1所述的成像镜头,其特征在于,所述第四透镜在光轴上的中心厚度CT4、所述第四透镜的物侧面的曲率半径R41,以及,所述第四透镜的像侧面的曲率半径R42满足:0.5<CT4*(R42/R41)<3。
- 根据权利要求1所述的成像镜头,其特征在于,所述第三透镜的像侧面的曲率半径R32,与所述第四透镜的物侧面的曲率半径R41满足:0.5<R41/R32<5。
- 根据权利要求1所述的成像镜头,其特征在于,所述第四透镜和所述第五透镜的组合焦距f45,与所述第五透镜和所述第六透镜在光轴上的空间间隔T56满足:-100<f45/T56<-5。
- 根据权利要求1所述的成像镜头,其特征在于,微距对焦时所述第六透镜像侧面和所述成像面在光轴方向的距离BFLmin,与所述第一透镜物侧面和所述成像面在光轴方向的距离TTL满足:BFLmin/TTL>0.05。
- 一种摄像模组,其特征在于,由物侧至像侧依次包括:光阑、如权利要求1-11中任一所述的成像镜头,以及,成像面。
- 一种电子设备,其特征在于,包括前面板、中框、后盖,以及,如权利要求12所述的摄像模组,其中:所述前面板上设有显示屏,所述中框设置在所述前面板与所述后盖之间,所述后盖上设有摄像孔;所述摄像模组通过所述摄像孔设置在所述电子设备中,所述摄像模组中的所述成像镜头的光轴方向与所述电子设备的厚度方向平行。
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| CN114355579A (zh) * | 2022-03-11 | 2022-04-15 | 江西晶超光学有限公司 | 光学镜头、摄像模组及电子设备 |
| WO2023153076A1 (ja) * | 2022-02-09 | 2023-08-17 | ソニーグループ株式会社 | ズームレンズ、および撮像装置 |
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| CN112965205B (zh) * | 2021-02-26 | 2022-06-28 | 天津欧菲光电有限公司 | 成像透镜组、摄像模组、电子设备以及汽车 |
| CN113900230B (zh) * | 2021-10-13 | 2023-09-05 | 江西晶超光学有限公司 | 光学系统、摄像模组及电子设备 |
| CN113960754B (zh) * | 2021-10-26 | 2023-10-31 | 浙江舜宇光学有限公司 | 光学成像镜头 |
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| JP2016173438A (ja) * | 2015-03-17 | 2016-09-29 | キヤノン株式会社 | ズームレンズ |
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| CN121028357A (zh) * | 2025-10-31 | 2025-11-28 | 高视科技(苏州)股份有限公司 | 一种显微筒镜及显微系统 |
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