Patent Application
20250093623
The subject matter relates to field of optical imaging, and more particularly, to an optical system, a camera module, and an electronic device.
In recent years, electronic devices equipped with cameras, including portable information terminals such as smartphones, digital cameras, laptops, tablet computers, have developed rapidly, and people's requirement for high imaging quality is increasing. In order to provide users with better photographing experience, the optical system is required to have higher resolution and imaging quality, and the optical system also needs to adapt to photographing requirements in various environments, such as photographing in a low light environment such as a night scene, a rainy day, and starry sky.
However, it is usually necessary to increase a quantity of lenses to achieve higher resolution, which increases overall length of the optical system. Increasing an amount of light entering the optical system can meet the photographing requirements in various environments, that is, it is necessary to increase an aperture of the optical system. Thus, a structure of the optical system becomes more complex, a size of a camera module is increased, the overall length of the camera module is increased, and the camera module is inapplicable to electronic products with a light, thin, and compact design.
An object of the present application is to provide an optical system, a camera module, and an electronic device, the optical system satisfies the requirements of large aperture, miniaturization, and good imaging effect.
In order to achieve the object of the present application, the present application provides the following technical solutions:
In a first aspect, the present application provides an optical system. The optical system consists of six lenses having refractive power. From an object side to an image side along an optical axis, the six lenses sequentially include a first lens, a second lens, a third lens, a fourth lens, a fifth lens, and a sixth lens. The first lens has positive refractive power, and an object side surface and an image side surface of the first lens are convex near the optical axis. The second lens has negative refractive power, and an image side surface of the second lens is concave near the optical axis. The third lens has refractive power, an object side surface of the third lens is convex near the optical axis, and an image side surface of the third lens is concave near the optical axis. The fourth lens has negative refractive power, an object side surface of the fourth lens is concave near the optical axis, and an image side surface of the fourth lens is convex near the optical axis. The fifth lens has positive refractive power, and an object side surface of the fifth lens is convex near the optical lens. The sixth lens has negative refractive power, an object side surface of the sixth lens is convex near the optical axis, and an image side surface of the sixth lens is concave near the optical axis.
The optical system satisfies the relational expression: 1.9<FNO<2.3, 85 deg<FOV<100 deg, 1.1<TTL/ImgH<1.4, wherein, FNO is an aperture number of the optical system, FOV is a maximum field of view of the optical system, and ImgH is half of an image height corresponding to a maximum field of view of the optical system.
The first lens has positive refractive power, and the object side surface and image side surface of the first lens are both convex near the optical axis, which is favorable for shortening a total optical length of the optical system, compressing light direction of respective field of view, and reducing spherical aberration, thereby satisfying requirements of high image quality and small size of the optical system. It is also beneficial for improving the positive refractive power of the first lens so as to further provide a reasonable incident angle of light to guide the edge light. The second lens has negative refractive power, and the image side surface of the second lens is concave near the near optical axis, which is conducive to entry and deflection of the edge light and can reduce a desired deflection angle of the rear lens, thereby allowing the deflection angle of light on each lens to be more uniform, and effectively correcting the aberration of the edge field of view. The third lens has refractive power, the object side surface of the third lens is convex near the optical axis, and the image side surface of the third lens is concave near the optical axis, which is favorable for delaying the light entering the system via the front lens and delaying the angle. The fourth lens has negative refractive power, the object side surface of the fourth lens is concave near the optical axis, and the image side surface of the fourth lens is convex near the optical axis, which is favorable for correcting the spherical aberration, coma, and distortion generated by the first lens, second lens, and third lens. The fifth lens has positive refractive power, and the object side surface of the fifth lens is convex near the optical axis, which is favorable for reasonably constraining curvature radius of the fifth lens, thereby reducing tolerance sensitivity of the optical system, and reducing the risk of generation of stray light. The sixth lens has negative refractive power, the object side surface of the sixth lens is convex near the optical axis, and the image side surface of the sixth lens is concave near the optical axis, which is favorable for shortening the total length of the optical system, correcting aberrations, increasing an emitting angle of light to allow the optical system to have the characteristics of a large image surface, and improving the resolution of the optical system, thereby allowing the optical system to have better imaging quality.
By satisfying the relational expression: 1.9<FNO<2.3, the optical system may have the characteristics of a large aperture, and the optical system may have sufficient amount of incident light. Thus, the optical system may capture images with higher definition, and the optical system is suitable for photographing high quality images of low brightness space scenes such as night scenes and starry skies.
By satisfying the relationship expression: 85 deg<FOV<100 deg, the optical system may have a large field of view. Thus, the optical system may have the characteristics of high pixels and high definition.
By satisfying the relationship expression: 1.1<TTL/ImgH<1.4, the total optical length of the optical system may be reduced. Thus, the optical system may have ultra-thin characteristics, meet a requirement of miniaturization of the optical system, and have more advantages when shooting scenes at medium focus distances.
In a second aspect, the present application further provides a camera module. The lens module includes a photosensitive chip and the optical system mentioned in any one of embodiments of the first aspect, and the photosensitive chip is located on an image side of the optical system. A photosensitive surface of the photosensitive chip is located on an imaging surface of the optical system. The light of an object that passes through the lens and is incident on the photosensitive surface can be converted into an electrical signal of an image. The photosensitive chip may be a complementary metal oxide semiconductor (CMOS) or a charge-coupled device (CCD). The camera module can be an imaging module integrated in an electronic device or an independent lens. By adding the optical system provided by the present application to the camera module, a surface shape and refractive power of each lens in the optical system can be reasonably designed, so that the camera module can meet the requirements of large aperture, miniaturization, and good imaging effect.
In a third aspect, the present application further provides an electronic device. The electronic device includes a housing and the camera module mentioned in the second aspect, and the camera module is located in the housing. The electronic device includes but is not limited to an automobile, a monitor, a smart phone, a computer, and a smart watch. By adding the camera module provided by the present application to the electronic device, the electronic device can meet the requirements of large aperture, miniaturization, and good imaging effect.
Implementations of the present technology will now be described, by way of embodiment, with reference to the attached figures. Obviously, the drawings are only some embodiments of the present disclosure. For those ordinary skill in the art, other drawings can be obtained based on these drawings without creative work.
Implementations of the present disclosure will now be described, by way of embodiments, with reference to the above figures. The embodiments are obviously a portion but not all of the embodiments of the present application. Based on the embodiments of the present application, other embodiments obtained by ordinary skill in the art without creative work will still fall within the scope of protection of the present application.
In a first aspect, the present application provides an optical system. The optical system consists of six lenses having refractive power. From an object side to an image side along an optical axis, the six lenses sequentially include a first lens, a second lens, a third lens, a fourth lens, a fifth lens, and a sixth lens. The first lens has positive refractive power, and an object side surface and an image side surface of the first lens are convex near the optical axis. The second lens has negative refractive power, and an image side surface of the second lens is concave near the optical axis. The third lens has refractive power, an object side surface of the third lens is convex near the optical axis, and an image side surface of the third lens is concave near the optical axis. The fourth lens has negative refractive power, an object side surface of the fourth lens is concave near the optical axis, and an image side surface of the fourth lens is convex near the optical axis. The fifth lens has positive refractive power, and an object side surface of the fifth lens is convex near the optical lens. The sixth lens has negative refractive power, an object side surface of the sixth lens is convex near the optical axis, and an image side surface of the sixth lens is concave near the optical axis.
The optical system satisfies the relational expression: 1.9<FNO<2.3. Further, the optical system satisfies the relational expression: 2<FNO<2.2. Wherein, FNO is an aperture number of the optical system.
The optical system satisfies the relational expression: 85 deg<FOV<100 deg. Further, the optical system satisfies the relational expression: 877 deg<FOV<95 deg. Wherein, FOV is a maximum field of view of the optical system.
The optical system satisfies the relational expression: 1.1<TTL/ImgH<1.4. Further, the optical system satisfies the relational expression: 1.22<TTL/ImgH<1.35. Wherein, ImgH is half of an image height corresponding to a maximum field of view of the optical system.
The first lens has positive refractive power, and the object side surface and image side surface of the first lens are both convex near the optical axis, which is favorable for shortening a total optical length of the optical system, compressing light direction of respective field of view, and reducing spherical aberration, thereby satisfying requirements of high image quality and small size of the optical system. It is also beneficial for improving the positive refractive power of the first lens so as to further provide a reasonable incident angle of light to guide the edge light. The second lens has negative refractive power, and the image side surface of the second lens is concave near the near optical axis, which is conducive to entry and deflection of the edge light and may reduce a desired deflection angle of the rear lens, thereby allowing the deflection angle of light on each lens to be more uniform, and effectively correcting the aberration of the edge field of view. The third lens has refractive power, the object side surface of the third lens is convex near the optical axis, and the image side surface of the third lens is concave near the optical axis, which is favorable for delaying the light entering the system via the front lens and delaying the angle. The fourth lens has negative refractive power, the object side surface of the fourth lens is concave near the optical axis, and the image side surface of the fourth lens is convex near the optical axis, which is favorable for correcting the spherical aberration, coma, and distortion generated by the first lens, second lens, and third lens. The fifth lens has positive refractive power, and the object side surface of the fifth lens is convex near the optical axis, which is favorable for reasonably constraining curvature radius of the fifth lens, thereby reducing tolerance sensitivity of the optical system, and reducing the risk of generation of stray light. The sixth lens has negative refractive power, the object side surface of the sixth lens is convex near the optical axis, and the image side surface of the sixth lens is concave near the optical axis, which is favorable for shortening the total length of the optical system, correcting aberrations, increasing a light emitting to allow the optical system to have the characteristics of a large image surface, and improving the resolution of the optical system, thereby allowing the optical system to have better imaging quality.
By satisfying the relational expression: 1.9<FNO<2.3, the optical system may have the characteristics of a large aperture, and the optical system may have sufficient amount of incident light. Thus, the optical system can capture images with higher definition, and the optical system is suitable for photographing high quality images of low brightness space scenes such as night scenes and starry skies.
By satisfying the relationship expression: 85 deg<FOV<100 deg, the optical system may have a large field of view. Thus, the optical system may have the characteristics of high pixels and high definition.
By satisfying the relationship expression: 1.1<TTL/ImgH<1.4, the total optical length of the optical system may be reduced. Thus, the optical system may have ultra-thin characteristics, meet the requirement of miniaturization of the optical system, and have more advantages when shooting scenes at medium focus distances.
In one embodiment, the optical system satisfies the relational expression: 0.5<R11/f<1.1. Further, the optical system satisfies the relational expression: 0.6<R11/f<1. Wherein, R11 is a radius of curvature of an object side surface of the first lens at the optical axis, and f is an effective focal length of the optical system. By satisfying the above relational expression, the ratio of the radius of curvature of the object side surface of the first lens at the optical axis to the effective focal length of the optical system may be reasonably limited, which is favorable for controlling the curvature of the first lens within a reasonable range and reduce an incident angle of light on the object side surface of the first lens. Thus, the optical system may have good imaging quality.
In one embodiment, the optical system satisfies the relational expression: −1.1<R12/f<−0.5. Further, the optical system satisfies the relational expression: −1<R12/f<−0.6. Wherein, R12 is a radius of curvature of an image side surface of the first lens at the optical axis, and f is the effective focal length of the optical system. By satisfying the above relational expression, a ratio of the curvature radius of the image side surface of the first lens at the optical axis and the effective focal length of the optical system may be reasonably limited, so that a surface shape of the object side surface of first lens and a surface shape of the image side surface of the first lens are matched to quickly converge the light, thereby reducing an aperture of a head of the optical system and realizing miniaturization of the head of the optical system.
In one embodiment, the optical system satisfies the relational expression: 5<|R21/f. Further, the optical system satisfies the relational expression: 7<|R21/f. Wherein, R21 is the radius of curvature of the object side surface of the second lens at the optical axis, and f is the effective focal length of the optical system. By satisfying the above relational expression, a ratio of the radius of curvature of the object side surface of the second lens at the optical axis to the effective focal length of the optical system may be reasonably limited, which is favorable for extending the propagation distance of light in a small aperture so as to further improve the degree of miniaturization of the head of the optical system.
In one embodiment, the optical system satisfies the relational expression: 0.6<R22/f<1.3. Further, the optical system satisfies the relational expression: 0.77<R22/f<1.2. Wherein, R22 is the radius of curvature of the image side surface of the second lens at the optical axis, and f is the effective focal length of the optical system. By satisfying the above relational expression, a ratio of the radius of curvature of the image side surface of the second lens at the optical axis to the effective focal length of the optical system may be reasonably limited, so that the light may diffuse smoothly toward the image side, thereby avoiding introduction of large off-axis chromatic aberration. Thus, the imaging quality may be improved.
In one embodiment, the optical system satisfies the relational expression: 0.5<R31/f<1.2. Further, the optical system satisfies the relational expression: 0.6<R31/f<1.1. Wherein, R31 is a radius of curvature of an object side surface of the third lens at the optical axis, and f is the effective focal length of the optical system. By satisfying the above relational expression, the ratio of the radius of curvature of the object side surface of the third lens at the optical axis to the effective focal length of the optical system may be reasonably limited, so that the astigmatism of the third lens may be controlled within a reasonable range, thereby effectively balancing the astigmatism. Thus, the optical system may have good imaging quality.
In one embodiment, the optical system satisfies the relational expression: 0.6<R32/f<1.2. Further, the optical system satisfies the relational expression: 0.7<R32/f<1.1. Wherein, R32 is a radius of curvature of the image side surface of the third lens at the optical axis, and f is the effective focal length of the optical system. By satisfying the above relational expression, the object side surface and the image side surface of the third lens are similar in shape, thereby avoiding the introduction of on-axis aberrations, facilitating the flexible design of aspheric surfaces, and balancing off-axis aberrations. Thus, the imaging quality may be improved.
In one embodiment, the optical system satisfies the relational expression: −1<R41/f<−0.3. Further, the optical system satisfies the relational expression: −0.9<R41/f<−0.35. Wherein, R41 is a radius of curvature of the object side surface of the fourth lens at the optical axis, and f is the effective focal length of the optical system. By satisfying the above relational expression, the ratio of the radius of curvature of the object side surface of the fourth lens at the optical axis to the effective focal length of the optical system may be reasonably limited, so that the astigmatism of the fourth lens may be controlled within a reasonable range, and the incident angle of light on the image side surface of the fourth lens may be reduced. Thus, the optical system may have good imaging quality.
In one embodiment, the optical system satisfies the relational expression: −2.1<R42/f<−0.4. Further, the optical system satisfies the relational expression: −1.9<R42/f<−0.5. Wherein, R42 is a radius of curvature of the image side surface of the fourth lens at the optical axis, and f is the effective focal length of the optical system. By satisfying the above relational expression, the ratio of the radius of curvature of the image side surface of the fourth lens at the optical axis to the effective focal length of the optical system may be reasonably limited, so that the incident angle of the light on the image side surface of the fourth lens may be reduced, the on-axis back focus may be reduced, and the total length of the optical system may be shortened. Thus, the optical system may be miniaturized.
In one embodiment, the optical system satisfies the relational expression: 0.2<R51/f<0.8. Further, the optical system satisfies the relational expression: 0.3<R51/f<0.7. Wherein, R51 is a radius of curvature of the object side surface of the fifth lens at the optical axis, and f is the effective focal length of the optical system. By satisfying the above relational expression, the ratio of the radius of curvature of the object side surface of the fifth lens at the optical axis to the effective focal length of the optical system may be reasonably limited, further reducing the on-axis back focus, and shortening the total length of the optical system. Thus, the optical system may be miniaturized.
In one embodiment, the optical system satisfies the relationship: 2.5<|R521/f; further, the optical system satisfies the relationship: 3<|R521/f<30. Wherein, R52 is the radius of curvature of the image side surface of the fifth lens at the optical axis, and f is the effective focal length of the optical system. By satisfying the above relational expression, the ratio of the radius of curvature of the image side surface of the fifth lens at the optical axis to the effective focal length of the optical system may be reasonably limited, so that the fifth lens may effectively balance the astigmatism generated by the first lens to the fourth lens. Thus, the optical system may have good imaging quality.
In one embodiment, the optical system satisfies the relational expression: 0.2<R61/f<0.7. Further, the optical system satisfies the relational expression: 0.3<R61/f<0.6. Wherein, R61 is a radius of curvature of the object side surface of the sixth lens at the optical axis, and f is the effective focal length of the optical system. By satisfying the above relationship, the ratio of the radius of curvature of the object side surface of the sixth lens at the optical axis to the effective focal length of the optical system may be reasonably limited, which may allow the sixth lens to gently receive incident light, thereby reducing the introduction of aberrations. Thus, the optical system may have good imaging quality.
In one embodiment, the optical system satisfies the relational expression: 0.1<R62/f<0.35. Further, the optical system satisfies the relational expression: 0.15<R62/f<0.35. Wherein, R62 is a radius of curvature of the image side surface of the sixth lens at the optical axis, and f is the effective focal length of the optical system. By satisfying the above relationship, the ratio of the radius of curvature of the image side surface of the sixth lens at the optical axis to the effective focal length of the optical system may be reasonably limited, which may allow light to be gently emitted by the sixth lens, thereby reducing the introduction of aberrations. Thus, the optical system may have good imaging quality.
In one embodiment, the optical system satisfies the relational expression: 1<|R32/R41|<2. Further, the optical system satisfies the relational expression: 1<|R32/R41|<1.9. Wherein, R32 is a radius of curvature of the image side surface of the third lens at the optical axis, and R41 is the radius of curvature of the object side surface of the fourth lens at the optical axis. By satisfy the above relational expression, the ratio of the radius of curvature of the image side surface of the third lens at the optical axis to the radius of curvature of the object side surface of the fourth lens at the optical axis may be reasonably limited, which may control the spacing change of a gap between the third lens and the fourth lens, reduce the sensitivity of the third lens and the fourth lens during the production process, and balance the spherical chromatic aberration of the optical system. Thus, the imaging quality of the optical system may be improved.
In one embodiment, the optical system satisfies the relational expression: 0.3<|(R61+R62)/f6|<0.8. Further, the optical system satisfies the relational expression: 0.4<|(R61+R62)/f6|<0.7. Wherein, R61 is a radius of curvature of the object side surface of the sixth lens at the optical axis, R62 is a radius of curvature of the image side surface of the sixth lens at the optical axis, and f6 is the effective focal length of the sixth lens. By satisfying the above relational expression, the ratio of the sum of the radii of curvature of the object side surface and the image side surface of the sixth lens at the optical axis to the effective focal length of the sixth lens may be reasonably limited, so that the astigmatism of the sixth lens is controlled within a reasonable range, effectively balancing the astigmatism generated by the first lens to the fifth lens, and improving the imaging quality of the optical system.
In one embodiment, the optical system satisfies the relational expression: 0.6<f1/f<0.9. Further, the optical system satisfies the relational expression: 0.65<f1/f<0.85. Wherein, f1 is the effective focal length of the first lens, and f is the effective focal length of the optical system. By satisfying the above relationship, the ratio of the effective focal length of the first lens to the effective focal length of the optical system may be reasonably limited. For the entire optical system, the refractive power of the first lens will not be too strong, thereby avoiding the introduction of excessive spherical aberration. Thus, the optical system may have good imaging quality.
In one embodiment, the optical system satisfies the relational expression: −1.6<f2/f<−1. Further, the optical system satisfies the relational expression: −1.5<f2/f<−1.1. Wherein, f2 is the effective focal length of the second lens, and f is the effective focal length of the optical system. By satisfying the above relationship, the ratio of the effective focal length of the second lens to the effective focal length of the optical system may be reasonably limited. For the entire optical system, the refractive power of the second lens will not be too strong, and the second lens may cooperate with the first lens to correct spherical aberration, so that the optical system may have good imaging quality.
In one embodiment, the optical system satisfies the relational expression: 7<f13|/f. Further, the optical system satisfies the relational expression: 9<|f3|/f<50. Wherein, f3 is the effective focal length of the third lens, and f is the effective focal length of the optical system. By satisfying the above relational expression, the ratio of the effective focal length of the third lens to the effective focal length of the optical system may reasonably limited, so that the spherical aberration and chromatic aberration may be further corrected. Thus, the optical system may have good imaging quality.
In one embodiment, the optical system satisfies the relational expression: −7<f4/f<−1. Further, the optical system satisfies the relational expression: −7<f4/f<−1.1. Wherein, f4 is the effective focal length of the fourth lens, and f is the effective focal length of the optical system. By satisfying the above relational expression, the ratio of the effective focal length of the fourth lens to the effective focal length of the optical system may be reasonably limited, so that the light may be gently diffused, the pressure of the subsequent lens to correct the aberration may be reduced, and the imaging quality may be improved.
In one embodiment, the optical system satisfies the relational expression: 0.5<f5/f<1.2. Further, the optical system satisfies the relational expression: 0.6<f5/f<1.1. Wherein, f5 is the effective focal length of the fifth lens, and f is the effective focal length of the optical system. By satisfying the above relational expression, the ratio of the effective focal length of the fifth lens to the effective focal length of the optical system may be reasonably limited. For the entire optical system, too large curvature of the surface shape caused by overload of the sixth lens may be avoided, so that the optical system has good imaging quality.
In one embodiment, the optical system satisfies the relational expression: −1.6<f6/f<−1. Further, the optical system satisfies the relational expression: −1.5<f6/f<−1.1. Wherein, f6 is the effective focal length of the sixth lens, and f is the effective focal length of the optical system. By satisfying the above relational expression, the ratio of the effective focal length of the sixth lens to the effective focal length of the optical system may be reasonably limited. For the entire optical system, the refractive power of the sixth lens may be appropriate, and the sixth lens may cooperate with the fifth lens to correct optical aberration, so that the optical system may have good imaging quality.
In one embodiment, the optical system satisfies the relational expression: 2<FNO*tan(HFOV)<2.4. Further, the optical system satisfies the relational expression: 2.1<FNO*tan(HFOV)<2.3. Wherein, FNO is the aperture number of the optical system, and HFOV is half of the maximum field of view of the optical system. By satisfying the above relational expression, the aperture number of the optical system and the maximum field of view of the optical system may be reasonably limited, so that the optical system may have the characteristics of a large aperture and large field of view, thereby improving clarity of the pixels and imaging surface of the optical system. Thus, the optical system may have better imaging quality.
In one embodiment, the optical system satisfies the relational expression: 3.8<f/SD11<4.5. Further, the optical system satisfies the relational expression: 4<f/SD11<4.3. Wherein, f is the effective focal length of the optical system, and SD11 is the maximum effective aperture of the object side surface of the first lens. By satisfying the above relational expression, the ratio of the effective focal length of the optical system to the maximum effective aperture of the object side surface of the first lens may be reasonably limited, that is, the relative amount of light entering the optical system may be kept within a reasonable range, and a large entrance pupil aperture may be achieved while satisfying small aperture of the first lens, thereby reducing the aperture number of the optical system. Thus, the amount of light entering the optical system may be improved, and a miniaturized design of the head of may be realized, so that the optical system may be more suitable for applications in under-screen cameras and low light scenes. When it is below the lower limit, the aperture of the first lens is too large, which is not conducive to miniaturization of the head. When it exceeds the upper limit, the amount of incident light is too small, and the image quality is poor under low light conditions.
In one embodiment, the optical system satisfies the relational expression: 1.1<CT1/SD11<1.4. Further, the optical system satisfies the relational expression: 1.1<CT1/SD11<1.3. Wherein, CT1 is a thickness of the first lens at the optical axis, and SD11 is the maximum effective aperture of the object side surface of the first lens. By satisfying the above relational expression, the first lens may satisfy the miniaturized design of the head, which is very suitable for applications in under-screen cameras and low light scenes. When it is below the lower limit, the aperture of the first lens is relatively large, which is not conducive to achieving a miniaturized design of the head. When it exceeds the upper limit, the thickness difference between a bearing area and an optical effective area is too large, which may result in a large thickness ratio of the lens to increase the manufacturing difficulty and is not conducive to improving yield.
In one embodiment, the optical system satisfies the relational expression: 0.6<ET1/CT1<0.9. Further, the optical system satisfies the relational expression: 0.65<ET1/CT1<0.8. Wherein, ET1 is a distance from a position where the object side surface of the first lens has the maximum effective aperture to a position where the image side surface of the first lens has the maximum effective aperture along the optical axis, and CT1 is a thickness of the first lens at the optical axis. By satisfying the above relational expression, the thickness and refractive power of the first lens in the direction perpendicular to the optical axis may be reasonably distributed. The first lens is a convex lens with a thick center and thin sides, and has positive refractive power, which may allow the first lens to shrink the incident light, thereby reducing the total optical length. Optionally, 0.82 mm<CT1<0.86 mm, the first lens may have a large edge thickness, which may allow the optical system to achieve a deeper head structure while meeting the requirements of a small head structure, so that the optical system may be suitable for shooting scenes with holes, such as full screen screens and under-screen cameras. When it is below the lower limit, the edge thickness of the first lens may small, and the depth of the head structure of the optical system may small, which cannot meet specific requirements of head depth. When it exceeds the upper limit, the refractive power of the first lens may be relatively small, making which cannot provide good deflection conditions for incident light and is not conducive to the contraction of light.
In one embodiment, the optical system satisfies the relational expression: 1<CT5/ET5<1.8. Further, the optical system satisfies the relational expression: 1.1<CT5/ET5<1.65. Wherein, CT5 is a thickness of the fifth lens at the optical axis, and ET5 is a distance from a position where the object side surface of the fifth lens has the maximum effective aperture to a position where the image side surface of the fifth lens has the maximum effective aperture along the optical axis. By satisfying the above relational expression, the edge thickness and center thickness of the fifth lens may be reasonably limited, the shape of the fifth lens may be controlled, and the spherical aberration, chromatic aberration, and field curvature of the optical system may be comprehensively balanced, and the imaging quality of the optical system may be improved.
In one embodiment, the optical system satisfies the relational expression: 0.8<ET6/CT6<1.3. Further, the optical system satisfies the relational expression: 0.85<ET6/CT6<1.2. Wherein, ET6 is a distance from a position where the object side surface of the sixth lens has the maximum effective aperture to a position where the image side surface of the sixth lens has the maximum effective aperture along the optical axis, and CT6 is a thickness of the sixth lens at the optical axis. By satisfying the above relational expression, the overall thickness of the sixth lens may be similar, so that the rear space of the optical system may be reasonably used, and manufacturing difficulty may be reduced. When it is below the lower limit, the proportion of edge thickness of the sixth lens may be small, and the supporting part is difficult to meet the thickness standard. When it exceeds the upper limit, the thickness of the sixth lens may be too large, which may cause the external support part to occupy too much space.
In one embodiment, the optical system satisfies the relational expression: 1<CT5/CT6<1.8. Further, the optical system satisfies the relational expression: 1<CT5/CT6<1.7. Wherein, CT5 is a thickness of the fifth lens at the optical axis, and CT6 is a thickness of the sixth lens at the optical axis. By satisfying the above relational expression, the distance between the fifth lens and the sixth lens may be reduced, which may improve compactness and may be conductive to the miniaturization of the optical system.
In one embodiment, the optical system satisfies the relational expression: 3<TD/CT1<4. Further, the optical system satisfies the relational expression: 3.3<TD/CT1<3.9. Wherein, TD is a distance from the object side surface of the first lens to the image side surface of the sixth lens along the optical axis, and CT1 is a thickness of the first lens at the optical axis. By satisfying the above relational expression, the miniaturized design of the head of the optical system may be satisfied to allow the thickness of the first lens to be matched with the optical system, which is favorable for reducing the sensitivity of the first lens, simplifying the processing and molding of the first lens, and achieving better engineering manufacturing.
In one embodiment, the optical system satisfies the relational expression: 0.5<AT56/AT23<1.8. Further, the optical system satisfies the relational expression: 0.6<AT56/AT23<1.7. Wherein, AT56 is a distance from the image side surface of the fifth lens to the object side surface of the sixth lens along the optical axis, and AT23 is a distance from the image side surface of the second lens to the object side surface of the third lens along the optical axis. By satisfying the above relational expression, the sensitivity of the second lens, third lens, fifth lens, and sixth lens may be reduced, the processing and molding of the second lens, third lens, fifth lens, and sixth lens may be simplified, and engineering manufacturing may be better achieved.
In one embodiment, the optical system satisfies the relational expression: 1<AT34/AT23<1.6. Further, the optical system satisfies the relational expression: 1<AT34/AT23<1.5. Wherein, AT23 is a distance from the image side surface of the second lens to the object side surface of the third lens along the optical axis, and AT34 is a distance from the image side surface of the third lens to the object side surface of the fourth lens along the optical axis. By satisfying the above relational expression, the sensitivity of the second lens, third lens, and fourth lens may be reduced, the processing and molding of the second lens, third lens, and fourth lens may be simplified, and engineering manufacturing may be better achieved.
In one embodiment, the optical system satisfies the relational expression: 4<T56max/T56min<11. Wherein, T56max is the maximum distance parallel to the optical axis between the fifth lens and the sixth lens, and T56min is the minimum distance parallel to the optical axis between the fifth lens and the sixth lens. By satisfying the above relational expression, a ratio of the maximum distance parallel to the optical axis between the fifth and sixth lenses to the minimum distance parallel to the optical axis between the fifth and sixth lenses may be reasonably limited, so that sizes and refractive powers of the fifth and sixth lenses may be reasonably limited, and the degree of curvature of the fifth and sixth lenses may be maintained within a reasonable range, thereby effectively reducing the astigmatism generated by the fifth and sixth lenses, reducing the overall sensitivity of the optical system, and facilitating the production and manufacturing of the fifth and sixth lenses.
In one embodiment, the optical system satisfies the relational expression: 0.2<(SAG11+SAG21)/TTL<0.3. Wherein, SAG11 is a distance from an intersection point of the object side surface of the first lens and the optical axis to a position where the image side surface of the first lens has the maximum effective aperture of along the optical axis, SAG21 is a distance from an intersection point of the object side surface of the second lens and the optical axis to a position where the image side surface of the second lens has the maximum effective aperture of along the optical axis, and TTL is a distance from the object side surface of the first lens to the imaging surface of the optical system along the optical axis. By satisfying the above relational expression, the thicknesses of the first and second lenses may be reasonably controlled, that is, a structural proportion of the thicker first and second lenses in the optical system may be controlled, thereby effectively reducing the total optical length of the optical system and achieving miniaturization.
In one embodiment, the optical system satisfies the relational expression: 4<L42/(W4+V4)<5. Wherein, L42 is half of the maximum effective aperture of the image side surface of the fourth lens, W4 is half of the maximum thickness of the fourth lens, and V4 is half of the minimum thickness of the fourth lens. By satisfying the above relational expression, the curvature of the fourth lens may be reasonably limited, which is favorable for balancing the aberrations of the optical system, reducing the sensitivity during the production process of the fourth lens, and improving the imaging quality of the optical system. When it is below the lower limit, the sensitivity during the production process of the fourth lens may be increased, which is not conducive to the production and manufacturing of the fourth lens. When it exceeds the upper limit, the fourth lens may be difficult to correct the field curvature aberration of the optical system, which affects the imaging quality of the optical system.
In one embodiment, the optical system satisfies the relational expression: 4<L62/(W6+V6)<6. Wherein, L62 is half of the maximum effective aperture of the image side surface of the sixth lens, W6 is half of the maximum thickness of the sixth lens, and V6 is half of the minimum thickness of the sixth lens. By satisfying the above relational expression, the curvature of the sixth lens may be reasonably limited, which is favorable for balancing the aberrations of the optical system, reducing the sensitivity during the production process of the sixth lens, and improving the imaging quality of the optical system. When it is below the lower limit, the sensitivity during the production process of the sixth lens may be increased, which is not conducive to the production and manufacturing of the sixth lens. When it exceeds the upper limit, the sixth lens may be difficult to correct the field curvature aberration of the optical system, which affects the imaging quality of the optical system.
In some embodiments, the optical system further includes an optical filter. The optical filter may be an infrared cut-off filter or an infrared bandpass filter. The infrared cut-off filter is used to filter out infrared light. The infrared bandpass filter only allows infrared light to pass through. In this application, the optical filter is an infrared cut-off filter, which is fixedly arranged relative to each lens in the optical system and is configured to prevent infrared light from reaching the imaging surface of the optical system and interfering with normal imaging. The optical filter can be assembled with each lens as a part of the optical system. In other embodiments, the optical filter can also be an independent component of the optical system. The optical filter can be installed between the optical system and the photosensitive chip during the assembly of the optical system and the photosensitive chip. The optical filter may be made of optical glass with coating. The optical filter may also be made of colored glass. The optical filter may also be made of other materials, which are selected according to actual needs. In other embodiments, the filtering effect of infrared light can also be achieved by setting a filter coating on at least one of the first to sixth lenses.
Referring to
The first lens L1 has positive refractive power, an object side surface S1 of the first lens L1 is ex near an optical axis, and an image side surface S2 of the first lens L1 is convex near the optical axis.
The second lens L2 has negative refractive power, an object side surface S3 of the second lens L2 is concave near the optical axis, and an image side surface S4 of the second lens L2 is concave near the optical axis.
The third lens L3 has negative refractive power, an object side surface S5 of the third lens L3 is convex near the optical axis, and an image side surface S6 of the third lens L3 is concave near the optical axis.
The fourth lens L4 has negative refractive power, and an object side surface S7 of the fourth lens L4 is concave near the optical axis, and an image side surface S8 of the fourth lens L4 is convex near the optical axis.
The fifth lens L5 has positive refractive power, an object side surface S9 of the fifth lens L5 is convex near the optical axis, and an image side surface S10 of the fifth lens L5 is convex near the optical axis.
The sixth lens L6 has negative refractive power, an object side surface S11 of the sixth lens L6 is convex near the optical axis, and an image side surface S12 of the sixth lens L5 is concave near the optical axis.
Moreover, the optical system also includes an aperture stop STO, an optical filter IR, and an imaging surface IMG. In this embodiment, the aperture stop STO is arranged on the object side surface of the first lens L1 and is configured to control the amount of incident light. The optical filter IR is arranged between the sixth lens L6 and the imaging surface IMG and includes an object side surface S13 and an image side surface S14. The optical filter IR is an infrared cut-off filter, which is used to filter out infrared light, so that the light entering the imaging surface IMG is visible light, and a wavelength of the visible light is in a range of 380 nm to 780 nm. The infrared cut-off filter may be made of glass or plastic, which can be coated thereon. The first lens L1 to the sixth lens L6 may be made of glass or plastic. An effective pixel area of the photosensitive chip is located on the imaging surface, and the photosensitive chip is set at the imaging surface IMG. The photosensitive chip captures different wavelength information of an object for subsequent processing.
Table 1a shows parameters of the optical system 10 of the embodiment. The Y radius in Table 1a is the radius of curvature of the object side surface or image side surface with the corresponding surface number at the optical axis. The surface numerals S1 and S2 are the object side surface S1 and image side surface S2 of the first lens L1, respectively. That is, for a same lens, the surface with a smaller surface numeral is the object side surface of the lens, and the surface with a larger surface is the image side surface of the lens. In a “thickness” column of the first lens L1, the first value is the thickness of the lens at the optical axis, and the second value is the distance from the image side surface of the lens to the next surface at the optical axis along a direction toward the image side. The focal length, material refractive index and Abbe number are obtained using visible light with a reference wavelength of 555 nm, and the units of the Y radius, thickness, and focal length are millimeters (mm).
Wherein, f is the focal length of the optical system 10, FNO is the aperture number of the optical system 10, FOV is the maximum field of view of the optical system 10. TTL is the distance from the object side surface of the first lens to the imaging surface along the optical axis, that is the total optical length.
In this embodiment, object side surfaces and the image side surfaces of the first lens L1 to the sixth lens L6 are all aspherical surfaces. The surface shape x of aspherical surface may be expressed by, but not limited to, the following aspherical formula:
Wherein, x is a distance from a corresponding point of the aspherical surface to a plane tangent to the vertex, h is a distance from any point on the aspherical surface to the optical axis 101, c is a curvature of a vertex of the aspherical surface, k is cone constant, and Ai is a coefficient corresponding to the ith higher-order term in the above aspherical formula. Table 1b shows the coefficients of high-order terms A4, A6, A8, A10, A12, A14, A16, A18, A20, A22, A24, A26, A28, A30 of the aspheric mirrors S1, S2, S3, S4, S5, S6, S7, S8, S9, S10, S11, S12 that can be used in the first embodiment.
Referring to (a) of
Referring to (b) of
Referring to (c) of
From (a), (b), and (c) of
Referring to
The first lens L1 has positive refractive power, an object side surface S1 of the first lens L1 is convex near an optical axis, and an image side surface S2 of the first lens L1 is convex near the optical axis.
The second lens L2 has negative refractive power, an object side surface S3 of the second lens L2 is convex near the optical axis, and an image side surface S4 of the second lens L2 is concave near the optical axis.
The third lens L3 has negative refractive power, an object side surface S5 of the third lens L3 is convex near the optical axis, and an image side surface S6 of the third lens L3 is concave near the optical axis.
The fourth lens L4 has negative refractive power, and an object side surface S7 of the fourth lens L4 is concave near the optical axis, and an image side surface S8 of the fourth lens L4 is convex near the optical axis.
The fifth lens L5 has positive refractive power, an object side surface S9 of the fifth lens L5 is convex near the optical axis, and an image side surface S10 of the fifth lens L5 is concave near the optical axis.
The sixth lens L6 has negative refractive power, an object side surface S11 of the sixth lens L6 is convex near the optical axis, and an image side surface S12 of the sixth lens L5 is concave near the optical axis.
The other structures of the optical system of the second embodiment are identical with the optical system of the second embodiment, reference can be made to the optical system of second embodiment.
Table 2a shows parameters of the optical system 10 of the embodiment. The focal length, material refractive index and Abbe number are obtained using visible light with a reference wavelength of 555 nm, the units of the Y radius, thickness, and focal length are millimeters (mm), and other parameters represent the same meaning as that in the first embodiment.
Wherein, f is the focal length of the optical system 10, FNO is the aperture number of the optical system 10, FOV is the maximum field of view of the optical system 10. TTL is the distance from the object side surface of the first lens to the imaging surface along the optical axis, that is the total optical length.
Table 2b shows the coefficients of high-order terms that can be used for each aspherical mirror surface in the second embodiment, wherein each aspherical surface shape can be defined by the formula provided in the first embodiment.
(a), (b), and (c) of
Referring to
The first lens L1 has positive refractive power, an object side surface S1 of the first lens L1 is convex near an optical axis, and an image side surface S2 of the first lens L1 is convex near the optical axis.
The second lens L2 has negative refractive power, an object side surface S3 of the second lens L2 is convex near the optical axis, and an image side surface S4 of the second lens L2 is concave near the optical axis.
The third lens L3 has negative refractive power, an object side surface S5 of the third lens L3 is convex near the optical axis, and an image side surface S6 of the third lens L3 is concave near the optical axis.
The fourth lens L4 has negative refractive power, and an object side surface S7 of the fourth lens L4 is concave near the optical axis, and an image side surface S8 of the fourth lens L4 is convex near the optical axis.
The fifth lens L5 has positive refractive power, an object side surface S9 of the fifth lens L5 is convex near the optical axis, and an image side surface S10 of the fifth lens L5 is concave near the optical axis.
The sixth lens L6 has negative refractive power, an object side surface S11 of the sixth lens L6 is convex near the optical axis, and an image side surface S12 of the sixth lens L5 is concave near the optical axis.
The other structures of the optical system of the third embodiment are identical with the optical system of the second embodiment, reference can be made to the optical system of first embodiment.
Table 3a shows parameters of the optical system 10 of the embodiment. The focal length, material refractive index and Abbe number are obtained using visible light with a reference wavelength of 555 nm, the units of the Y radius, thickness, and focal length are millimeters (mm), and other parameters represent the same meaning as that in the first embodiment.
Wherein, f is the focal length of the optical system 10, FNO is the aperture number of the optical system 10, FOV is the maximum field of view of the optical system 10. TTL is the distance from the object side surface of the first lens to the imaging surface along the optical axis, that is the total optical length.
Table 3b shows the coefficients of high-order terms that can be used for each aspherical mirror surface in the third embodiment, wherein each aspherical surface shape can be defined by the formula provided in the first embodiment.
(a), (b), and (c) of
Referring to
The first lens L1 has positive refractive power, an object side surface S1 of the first lens L1 is convex near an optical axis, and an image side surface S2 of the first lens L1 is convex near the optical axis.
The second lens L2 has negative refractive power, an object side surface S3 of the second lens L2 is convex near the optical axis, and an image side surface S4 of the second lens L2 is concave near the optical axis.
The third lens L3 has positive refractive power, an object side surface S5 of the third lens L3 is convex near the optical axis, and an image side surface S6 of the third lens L3 is concave near the optical axis.
The fourth lens L4 has negative refractive power, and an object side surface S7 of the fourth lens L4 is concave near the optical axis, and an image side surface S8 of the fourth lens L4 is convex near the optical axis.
The fifth lens L5 has positive refractive power, an object side surface S9 of the fifth lens L5 is convex near the optical axis, and an image side surface S10 of the fifth lens L5 is convex near the optical axis.
The sixth lens L6 has negative refractive power, an object side surface S11 of the sixth lens L6 is convex near the optical axis, and an image side surface S12 of the sixth lens L5 is concave near the optical axis.
Table 4a shows parameters of the optical system 10 of the embodiment. The focal length, material refractive index and Abbe number are obtained using visible light with a reference wavelength of 555 nm, the units of the Y radius, thickness, and focal length are millimeters (mm), and other parameters represent the same meaning as that in the first embodiment.
Wherein, f is the focal length of the optical system 10, FNO is the aperture number of the optical system 10, FOV is the maximum field of view of the optical system 10. TTL is the distance from the object side surface of the first lens to the imaging surface along the optical axis, that is the total optical length.
Table 4b shows the coefficients of high-order terms that can be used for each aspherical mirror surface in the fourth embodiment, wherein each aspherical surface shape can be defined by the formula provided in the first embodiment.
(a), (b), and (c) of
Referring to
The first lens L1 has positive refractive power, an object side surface S1 of the first lens L1 is convex near an optical axis, and an image side surface S2 of the first lens L1 is convex near the optical axis.
The second lens L2 has negative refractive power, an object side surface S3 of the second lens L2 is concave near the optical axis, and an image side surface S4 of the second lens L2 is concave near the optical axis.
The third lens L3 has positive refractive power, an object side surface S5 of the third lens L3 is convex near the optical axis, and an image side surface S6 of the third lens L3 is concave near the optical axis.
The fourth lens L4 has negative refractive power, and an object side surface S7 of the fourth lens L4 is concave near the optical axis, and an image side surface S8 of the fourth lens L4 is convex near the optical axis.
The fifth lens L5 has positive refractive power, an object side surface S9 of the fifth lens L5 is convex near the optical axis, and an image side surface S10 of the fifth lens L5 is concave near the optical axis.
The sixth lens L6 has negative refractive power, an object side surface S11 of the sixth lens L6 is convex near the optical axis, and an image side surface S12 of the sixth lens L5 is concave near the optical axis.
Table 5a shows parameters of the optical system 10 of the embodiment. The focal length, material refractive index and Abbe number are obtained using visible light with a reference wavelength of 555 nm, the units of the Y radius, thickness, and focal length are millimeters (mm), and other parameters represent the same meaning as that in the first embodiment.
Wherein, f is the focal length of the optical system 10, FNO is the aperture number of the optical system 10, and FOV is the maximum field of view of the optical system 10. TTL is the distance from the object side surface of the first lens to the imaging surface along the optical axis, that is the total optical length.
Table 5b shows the coefficients of high-order terms that can be used for each aspherical mirror surface in the fifth embodiment, wherein each aspherical surface shape can be defined by the formula provided in the first embodiment.
(a), (b), and (c) of
Referring to
The first lens L1 has positive refractive power, an object side surface S1 of the first lens L1 is convex near an optical axis, and an image side surface S2 of the first lens L1 is convex near the optical axis.
The second lens L2 has negative refractive power, an object side surface S3 of the second lens L2 is convex near the optical axis, and an image side surface S4 of the second lens L2 is concave near the optical axis.
The third lens L3 has positive refractive power, an object side surface S5 of the third lens L3 is convex near the optical axis, and an image side surface S6 of the third lens L3 is concave near the optical axis.
The fourth lens L4 has negative refractive power, and an object side surface S7 of the fourth lens L4 is concave near the optical axis, and an image side surface S8 of the fourth lens L4 is convex near the optical axis.
The fifth lens L5 has positive refractive power, an object side surface S9 of the fifth lens L5 is convex near the optical axis, and an image side surface S10 of the fifth lens L5 is concave near the optical axis.
The sixth lens L6 has negative refractive power, an object side surface S11 of the sixth lens L6 is convex near the optical axis, and an image side surface S12 of the sixth lens L5 is concave near the optical axis.
Table 6a shows parameters of the optical system 10 of the embodiment. The focal length, material refractive index and Abbe number are obtained using visible light with a reference wavelength of 555 nm, the units of the Y radius, thickness, and focal length are millimeters (mm), and other parameters represent the same meaning as that in the first embodiment.
Wherein, f is the focal length of the optical system 10, FNO is the aperture number of the optical system 10, and FOV is the maximum field of view of the optical system 10. TTL is the distance from the object side surface of the first lens to the imaging surface along the optical axis, that is the total optical length.
Table 6b shows the coefficients of high-order terms that can be used for each aspherical mirror surface in the sixth embodiment, wherein each aspherical surface shape can be defined by the formula provided in the first embodiment.
(a), (b), and (c) of
Table 7 shows values of FNO, FOV, TTL/ImgH, R11/f, R12/f, |R21|/f, R22/f, R31/f, R32/f, R41/f, R42/f, R51/f, |R52|/f, R61/f, R62/f, f1/f, f2/f, |f3|/f, f4/f, f5/f, f6/f, FNO*tan(HFOV), f/SD11, CT1/SD11, ET1/CT1, CT5/ET5, ET6/CT6, CT5/CT6, TD/CT1, AT56/AT23, AT34/AT23, (SAG11+SAG21)/TTL, |R32/R411, |(R61+R62)/f6|, L42/(W4+V4), L62/(W6+V6), T56max/T56min of the optical systems of the first embodiment to the sixth embodiment.
It can be seen from table 7, the optical systems of firs to sixth embodiments satisfy the following relational expressions: 1.9<FNO<2.3, 85 deg<FOV<100 deg, 1.1<TTL/ImgH<1.4, 0.5<R11/f<1.1, −1.1<R12/f<−0.5, 5<|R21|/f, 0.6<R22/f<1.3, 0.5<R31/f<1.2, 0.6<R32/f<1.2, −0.6<f1/f<0.9, −1.6<f2/f<−1, 7<−1/f, −7<f4/f<−1, 0.5<f5/f<1.2, −1.6<f6/f<−1, 2<FNO*tan(HFOV)<2.4, 3.8<f/SD11<4.5, 1.1<CT1/SD11<1.4, 0.6<ET1/CT1<0.9, 1<CT5/ET5<1.8, 0.8<ET6/CT6<1.3, 1<CT5/CT6<1.8, 3<TD/CT1<4, 0.5<AT56/AT23<1.8, 1<AT34/AT23<1.6, 0.2<(SAG11+SAG21)/TTL<0.3, 1<|R32/R41|<2, 0.3<|(R61+R62)/f6|<0.8, 4<L42/(W4+V4)<5, 4<L62/(W6+V6)<6, 4<T56max/T56min<11.
Referring to
Referring to
The above embodiments are only for describing but not intended to limit the present disclosure. Although the embodiments of the present disclosure have been described, those having ordinary skill in the art can understand that changes may be made within the principles of the present disclosure, up to and including the full extent established by the broad general meaning of the terms used in the claims. It will, therefore, be appreciated that the embodiments described above may be modified within the scope of the claims.
| Number | Date | Country | Kind |
|---|---|---|---|
| 202311211261.3 | Sep 2023 | CN | national |
