TWI650578B - Optical imaging system (1) - Google Patents

Abstract

An optical imaging system includes a first lens, a second lens, a third lens, a fourth lens, a fifth lens, a sixth lens, and a seventh lens in this order from the object side to the image side. At least one of the first to sixth lenses has a positive refractive power. The seventh lens may have a negative refractive power, and both surfaces thereof are aspherical, and at least one surface of the seventh lens has a point of inflection. The lenses with refractive power in the optical imaging system are the first lens to the seventh lens. When certain conditions are met, it can have greater light collection and better light path adjustment capabilities to improve imaging quality.

Description

Optical imaging system (1)

The invention relates to an optical imaging system group, and more particularly to a miniaturized optical imaging system group applied to electronic products.

In recent years, with the rise of portable electronic products with photographic functions, the demand for optical systems has been increasing. The photosensitive elements of general optical systems are nothing more than two types: photosensitive coupled device (CCD) or complementary metal-Oxide Semiconductor sensor (CMOS sensor), and with the advancement of semiconductor process technology, The pixel size of the photosensitive element is reduced, and the optical system is gradually developed in the high pixel field, so the requirements for imaging quality are also increasing.

Traditionally, the optical system mounted on portable devices mainly uses five or six lens structures. However, as portable devices continue to improve pixel quality and end consumers ’demands for large apertures such as low light and night light Shooting function, the conventional optical imaging system has been unable to meet higher-level photography requirements.

Therefore, how to effectively increase the amount of light entering the optical imaging lens and further improve the imaging quality has become a very important issue.

The aspect of the embodiment of the present invention is directed to an optical imaging system and an optical image capturing lens, which can use the combination of the refractive power of seven lenses, a convex surface, and a concave surface (the convex surface or concave surface in the present invention refers to the object side of each lens in principle). Or like the description of the change of the geometric shape at different heights from the optical axis to the side), which can effectively increase the amount of light entering the optical imaging system and improve the imaging quality at the same time, so that it can be applied to small electronic products.

In addition, in specific optical imaging applications, there is a need to target both visible light and Light sources with infrared wavelengths, such as IP video surveillance cameras. The "Day & Night" feature of IP video surveillance cameras is mainly because human visible light is located in the spectrum of 400-700nm, but the imaging of the sensor includes human invisible infrared light, so in order to ensure that The sensor finally retains only the visible light of the human eye. If necessary, a removable IR cut filter (ICR) is set in front of the lens to increase the "realism" of the image, which can eliminate infrared during the daytime. Light and avoid color shift; let infrared light come in at night to increase brightness. However, the ICR element itself occupies a considerable volume and is expensive, which is disadvantageous for the design and manufacture of future miniature surveillance cameras.

The aspect of the embodiment of the present invention is directed to an optical imaging system and an optical image capturing lens. The refractive power of seven lenses, the combination of convex and concave surfaces, and the selection of materials can be used to make the optical imaging system focus on visible light and infrared light. The gap between the imaging focal lengths is reduced, that is, it is close to the "confocal" effect, so there is no need to use ICR components.

The terms of the lens parameters and their codes related to the embodiments of the present invention are listed in detail below as a reference for subsequent descriptions:

Lens parameters related to the magnification of optical imaging systems and optical image capture lenses

The optical imaging system and the optical image capturing lens of the present invention can also be designed for biometric identification, such as facial recognition. If the embodiment of the present invention is used for image capture of face recognition, infrared light may be used as the working wavelength. At the same time, for faces with a distance of about 25 to 30 cm and a width of about 15 cm, it can be applied to the photosensitive element (pixel size 1.4 micrometers (μm)) at least 30 horizontal pixels are imaged in the horizontal direction. The linear magnification of the infrared imaging surface is LM, which meets the following conditions: LM = (30 horizontal pixels) multiplied by (pixel size of 1.4 microns) divided by the width of the subject 15 cm; LM ≧ 0.0003. At the same time, visible light is used as the working wavelength. At the same time, at least 50 faces with a distance of about 25 to 30 cm and a width of about 15 cm can be imaged horizontally on a photosensitive element (pixel size is 1.4 micrometers (μm)). Horizontal pixels.

Lens parameters related to length or height

In the present invention, a wavelength of 555 nm can be selected as a main reference wavelength and a reference for measuring focus shift in the visible light spectrum, and a wavelength of 850 nm can be selected as a main reference wavelength and a reference for measuring focus shift in the infrared light spectrum (700 nm to 1300 nm).

The optical imaging system has a first imaging plane and a second imaging plane. The first imaging plane is a visible light image plane perpendicular to the optical axis, and the central field of view is a defocus modulation conversion contrast transfer rate at a first spatial frequency. (MTF) has a maximum value; and the second imaging plane is a specific perpendicular to the light The infrared light image plane of the axis and its central field of view at the first spatial frequency have a maximum defocus modulation conversion contrast transfer rate (MTF). The optical imaging system further has a first average imaging plane and a second average imaging plane. The first average imaging plane is a visible light image plane perpendicular to the optical axis and is set in the central field of view of the optical imaging system. The average position of the defocus position of the field and the 0.7 field of view each having the maximum MTF value of the field of view at the first spatial frequency; and the second average imaging plane is a specific infrared light image plane perpendicular to the optical axis and is set at The central field of view, the 0.3 field of view, and the 0.7 field of view of the optical imaging system each have an average position of an out-of-focus position having a maximum MTF value of each of the fields at a first spatial frequency.

The aforementioned first spatial frequency is set to a half of the spatial frequency (half frequency) of the photosensitive element (sensor) used in the present invention. For example, the pixel size is a photosensitive element containing 1.12 micrometers or less, and its modulation conversion function characteristic is The quarter space frequency, half space frequency (half frequency) and full space frequency (full frequency) of the figure are at least 110 cycles / mm, 220 cycles / mm, and 440 cycles / mm, respectively. The light in any field of view can be further divided into sagittal ray and tangential ray.

The focus offsets of the maximum defocus MTF of the sagittal rays of the visible light center field of view, 0.3 field of view, and 0.7 field of view of the optical imaging system of the present invention are respectively represented by VSFS0, VSFS3, and VSFS7 (unit of measurement: mm); visible light center The maximum defocus MTF of the sagittal plane rays of the field of view, 0.3 field of view, and 0.7 field of view are represented by VSMTF0, VSMTF3, and VSMTF7, respectively; the maximum defocus MTF of the meridional rays of the central field of view, 0.3 field of view, and 0.7 field of view The value of the focus offset is represented by VTFS0, VTFS3, and VTFS7 (measurement unit: mm); the maximum defocus MTF of the meridional rays of the central field of view, 0.3 field of view, and 0.7 field of view is VTMTF0, VTMTF3, and VTMTF7, respectively. Means. The average focus shift amount (position) of the aforementioned focus shift amounts of the sagittal view field of the visible light arc and the three view fields of the visible meridian plane is represented by AVFS (measurement unit: mm).

The focus offset of the maximum defocus MTF of the sagittal plane rays of the central field, the 0.3 field of view, and the 0.7 field of vision of the optical imaging system of the present invention is represented by ISFS0, ISFS3, and ISFS7, respectively. The average focus offset (position) of the focus offset is expressed in AISFS (measurement unit: mm); the maximum defocus MTF of the sagittal rays of the infrared central field, 0.3 field of view, and 0.7 field of view is ISMTF0, ISMTF3 and ISMTF7 are indicated; the focus offset of the maximum defocus MTF of the meridional rays of the central field of view, 0.3 field of view, and 0.7 field of view of the infrared light is represented by ITFS0, ITFS3, and ITFS7 (unit of measurement: mm), the aforementioned meridian The average focus offset (position) of the focus offset of the three fields of view is represented by AITFS (unit of measurement: mm); the center of view of the infrared light, 0.3 field of view, The maximum out-of-focus MTF of the meridional light in the 0.7 field of view is represented by IMTTF0, IMTTF3, and IMTTF7, respectively. The average focus shift amount (position) of the aforementioned focus shift amounts of the sagittal three-field of the infrared light arc and the three fields of the meridional infrared light plane is represented by AIFS (unit of measurement: mm).

The focus offset between the visible light center field focus point and the infrared light center field focus point (RGB / IR) of the entire optical imaging system is represented by FS (ie, wavelength 850nm vs. wavelength 555nm, unit of measurement: mm); the entire optical The difference between the visible focus three-field average focus offset and the infrared light three-field average focus offset (RGB / IR) of the imaging system (focus offset) is expressed in AFS (that is, a wavelength of 850 nm to a wavelength of 555 nm, Unit of measurement: mm).

The maximum imaging height of the optical imaging system is represented by HOI; the height of the optical imaging system is represented by HOS; the distance between the first lens object side and the seventh lens image side of the optical imaging system is represented by InTL; the fixed light bar of the optical imaging system ( The distance from the aperture to the first imaging surface is represented by InS; the distance between the first lens and the second lens of the optical imaging system is represented by IN12 (example); the thickness of the first lens of the optical imaging system on the optical axis is represented by TP1 Display (example).

Lens parameters related to materials

The dispersion coefficient of the first lens of the optical imaging system is represented by NA1 (illustration); the refraction law of the first lens is represented by Nd1 (illustration).

Angle-dependent lens parameters

The angle of view is represented by AF; half of the angle of view is represented by HAF; the principal ray angle is represented by MRA.

Lens parameters related to exit pupil

The diameter of the entrance pupil of an optical imaging system is represented by HEP; the maximum effective radius of any surface of a single lens refers to the point where the system ’s maximum viewing angle of incident light passes through the edge of the entrance pupil at the lens surface (Effective Half Diameter; EHD), The vertical height between the intersection and the optical axis. For example, the maximum effective radius of the object side of the first lens is represented by EHD11, and the maximum effective radius of the image side of the first lens is represented by EHD12. The maximum effective radius of the object side of the second lens is represented by EHD21, and the maximum effective radius of the image side of the second lens is represented by EHD22. The maximum effective radius of any surface of the remaining lenses in the optical imaging system is expressed in the same manner.

Parameters related to lens surface arc length and surface contour

The length of the contour curve of the maximum effective radius of any surface of a single lens refers to the starting point of the intersection of the surface of the lens and the optical axis of the optical imaging system to which it belongs, from the starting point along the surface contour of the lens to its Up to the end of the maximum effective radius, the arc length between the two points is the contour of the maximum effective radius The length of the curve, expressed in ARS. For example, the length of the contour curve of the maximum effective radius on the object side of the first lens is represented by ARS11, and the length of the contour curve of the maximum effective radius of the image side of the first lens is represented by ARS12. The length of the contour curve of the maximum effective radius on the object side of the second lens is represented by ARS21, and the length of the contour curve of the maximum effective radius of the image side of the second lens is represented by ARS22. The length of the contour curve of the maximum effective radius of any surface of the remaining lenses in the optical imaging system is expressed in the same manner.

The length of the contour curve of 1/2 of the entrance pupil diameter (HEP) of any surface of a single lens refers to the intersection of the surface of the lens and the optical axis of the optical imaging system to which it belongs as the starting point. The surface contour of the lens is up to the coordinate point of the vertical height of 1/2 of the entrance pupil diameter from the optical axis on the surface. The curve arc length between the two points is 1/2 the length of the contour curve of the entrance pupil diameter (HEP). ARE said. For example, the contour curve length of 1/2 incident pupil diameter (HEP) on the object side of the first lens is represented by ARE11, and the contour curve length of 1/2 incident pupil diameter (HEP) on the image side of the first lens is represented by ARE12. The length of the profile curve of 1/2 incident pupil diameter (HEP) on the object side of the second lens is represented by ARE21, and the length of the profile curve of 1/2 incident pupil diameter (HEP) on the image side of the second lens is represented by ARE22. The contour curve length of 1/2 of the entrance pupil diameter (HEP) of any surface of the remaining lenses in the optical imaging system is expressed in the same manner.

Parameters related to lens surface depth

The intersection of the seventh lens object side on the optical axis to the end of the maximum effective radius of the seventh lens object side. The distance between the two points horizontal to the optical axis is represented by InRS71 (the maximum effective radius depth); the seventh lens image side From the intersection point on the optical axis to the end of the maximum effective radius of the image side of the seventh lens, the distance between the two points horizontal to the optical axis is represented by InRS72 (the maximum effective radius depth). The depth (sinking amount) of the maximum effective radius of the object side or image side of other lenses is expressed in the same manner as described above.

Parameters related to lens shape

The critical point C refers to a point on a specific lens surface that is tangent to a tangent plane that is perpendicular to the optical axis except for the intersection with the optical axis. For example, the vertical distance between the critical point C51 on the object side of the fifth lens and the optical axis is HVT51 (example), the vertical distance between the critical point C52 on the image side of the fifth lens and the optical axis is HVT52 (example), and the sixth lens object The vertical distance between the critical point C61 on the side and the optical axis is HVT61 (illustrated), and the vertical distance between the critical point C62 on the side of the sixth lens image and the optical axis is HVT62 (illustrated). The critical points on the object side or the image side of other lenses, such as the seventh lens, and the vertical distance from the optical axis are expressed in the same manner as described above.

The inflection point closest to the optical axis on the object side of the seventh lens is IF711, and the amount of subsidence at this point SGI711 (for example), SGI711 is the horizontal displacement distance parallel to the optical axis between the intersection of the seventh lens object side on the optical axis and the closest optical axis inflection point on the seventh lens object side. The vertical distance is HIF711 (example). The inflection point on the image side of the seventh lens that is closest to the optical axis is IF721. This point sinks SGI721 (for example). SGI711 is the intersection of the seventh lens image side on the optical axis and the closest optical axis of the seventh lens image side. The horizontal displacement distance between the inflection points parallel to the optical axis, and the vertical distance between this point of IF721 and the optical axis is HIF721 (illustration).

The second inflection point on the object side of the seventh lens approaching the optical axis is IF712. This point has a subsidence of SGI712 (for example). SGI712, that is, the intersection of the object side of the seventh lens on the optical axis, is the second closest to the object side of the seventh lens. The horizontal displacement distance between the inflection points of the optical axis and the optical axis is parallel. The vertical distance between this point of the IF712 and the optical axis is HIF712 (example). The second inflection point on the seventh lens image side that is close to the optical axis is IF722. This point has a subsidence of SGI722 (for example). SGI722 is the intersection of the seventh lens image side on the optical axis and the seventh lens image side is the second closest. The horizontal displacement distance between the inflection points of the optical axis and the optical axis is parallel, and the vertical distance between this point and the optical axis of IF722 is HIF722 (illustration).

The third inflection point on the object side of the seventh lens approaching the optical axis is IF713. This point has a subsidence of SGI713 (for example). SGI713, that is, the intersection of the object side of the seventh lens on the optical axis is the third closest to the object side of the seventh lens The horizontal displacement distance between the inflection points of the optical axis and the optical axis is parallel, and the vertical distance between this point and the optical axis of IF713 is HIF713 (illustration). The third inflection point on the seventh lens image side close to the optical axis is IF723, which is the amount of subsidence SGI723 (for example), SGI723, that is, the intersection of the seventh lens image side on the optical axis to the seventh lens image side third approach The horizontal displacement distance between the inflection points of the optical axis is parallel to the optical axis, and the vertical distance between this point of the IF723 and the optical axis is HIF723 (example).

The inflection point of the fourth lens close to the optical axis on the seventh lens object side is IF714. This point has a subsidence of SGI714 (for example). SGI714, that is, the intersection of the seventh lens object side on the optical axis and the seventh lens object side is fourth closer. The horizontal displacement distance between the inflection points of the optical axis is parallel to the optical axis. The vertical distance between this point and the optical axis of IF714 is HIF714 (illustration). The inflection point on the seventh lens image side close to the optical axis is IF724, which is the amount of subsidence SGI724 (for example). SGI724, that is, the intersection of the seventh lens image side on the optical axis to the seventh lens image side fourth approach The horizontal displacement distance between the inflection points of the optical axis and the optical axis is parallel. The vertical distance between this point and the optical axis of IF724 is HIF724 (illustration).

The inflection points on the object side or image side of other lenses and their vertical distance from the optical axis or the amount of their subsidence are expressed in the same manner as described above.

Aberration-related variables

Optical Distortion of an optical imaging system is represented by ODT; its TV Distortion is represented by TDT, and the degree of aberration shift between 50% and 100% of the field of view can be further defined; spherical aberration bias The amount of shift is expressed in DFS; the amount of comet aberration shift is expressed in DFC.

The lateral aberration of the aperture edge is expressed by STA (STOP Transverse Aberration). To evaluate the performance of a specific optical imaging system, you can use a tangential fan or a sagittal fan to calculate the horizontal direction of light in any field of view. Aberrations, in particular, the lateral aberrations of the longest operating wavelength (for example, a wavelength of 650NM) and the shortest operating wavelength (for example, a wavelength of 470NM) passing through the aperture edge are used as standards for excellent performance. The coordinate directions of the aforementioned meridional light fans can be further divided into positive (upper light) and negative (lower light) directions. The lateral aberration of the longest working wavelength passing through the edge of the aperture is defined as the imaging position where the longest working wavelength is incident on the first imaging plane through the edge of the aperture at a specific field of view. The distance between the two positions of the imaging position of the field of view on the plane. The shortest working wavelength passes through the lateral aberration of the aperture edge. It is defined as the imaging position where the shortest working wavelength is incident on a specific field of view on the first imaging plane through the edge of the aperture. The distance between the imaging position of the main field of the reference wavelength and the imaging position of the field of view on the first imaging plane. The performance of the specific optical imaging system is excellent. The shortest and longest working wavelength can be used to enter the first imaging plane through the aperture edge. The upper 0.7 field of view (that is, 0.7 imaging height HOI) has lateral aberrations less than 100 micrometers (μm) as a check method, and can further be incident on the first imaging surface with the shortest and longest working wavelength through the edge of the 0.7 field of view. The lateral aberrations are all less than 80 micrometers (μm) as the inspection method. The optical imaging system has a maximum imaging height HOI perpendicular to the optical axis on the first imaging plane. The longest working wavelength of the visible light of the positive meridional fan of the optical imaging system passes through the edge of the entrance pupil and is incident on the first imaging plane 0.7. The lateral aberration at HOI is represented by PLTA. The shortest working wavelength of the visible light of the positive meridional fan passes through the edge of the entrance pupil and incident on the first imaging plane. The lateral aberration at 0.7 HOI is represented by PSTA, and negative meridian. The longest working wavelength of the visible light of the surface light fan passes through the edge of the entrance pupil and the transverse aberration at 0.7HOI incident on the first imaging plane is represented by NLTA. The shortest working wavelength of the visible light of the negative meridional light fan passes through the edge of the entrance pupil and The lateral aberration at 0.7HOI incident on the first imaging plane is represented by NSTA. The longest working wavelength of the visible light of the sagittal plane fan passes through the edge of the entrance pupil and enters the lateral aberration at 0.7HOI on the first imaging plane. SLTA indicates that the shortest working wavelength of the visible light of the sagittal plane fan passes through the edge of the entrance pupil and is incident on the first imaging plane at 0.7HOI. The lateral aberration is represented by SSTA.

The invention provides an optical imaging system, which can simultaneously focus visible light and infrared (dual-mode) and achieve a certain performance, and the seventh lens has an inflection point on the object or image side, which can effectively adjust the incidence of each field of view. The angle of the seventh lens is corrected for optical distortion and TV distortion. In addition, the surface of the seventh lens may have better light path adjustment capabilities to improve imaging quality.

According to the present invention, an optical imaging system is provided, which includes a first lens, a second lens, a third lens, a fourth lens, a fifth lens, a sixth lens, a seventh lens, and a first imaging surface in this order from the object side to the image side. And a second imaging plane. The first imaging plane is a specific visible light image plane perpendicular to the optical axis, and the central field of view has a maximum defocus modulation conversion contrast transfer rate (MTF) at the first spatial frequency; the second imaging plane is a specific vertical The defocus modulation conversion contrast transfer rate (MTF) of the infrared light image plane at the optical axis and its central field of view at the first spatial frequency has a maximum value. Each of the first to seventh lenses has a refractive power. The material of at least one of the first lens to the seventh lens is plastic and the material of at least one lens is glass. The focal lengths of the first lens to the seventh lens are f1, f2, f3, f4, f5, f6, f7, the focal length of the optical imaging system is f, and the entrance pupil diameter of the optical imaging system is HEP. There is a distance HOS on the optical axis from the side of the lens object to the first imaging plane. Half of the maximum viewing angle of the optical imaging system is HAF. The optical imaging system has a maximum imaging perpendicular to the optical axis on the first imaging plane. For the height HOI, the distance on the optical axis between the first imaging surface and the second imaging surface is FS, which meets the following conditions: 1 ≦ f / HEP ≦ 10; 0deg <HAF ≦ 150deg; and | FS | ≦ 60 μm.

According to the present invention, there is also provided an optical imaging system, which sequentially includes a first lens, a second lens, a third lens, a fourth lens, a fifth lens, a sixth lens, a seventh lens, and a first image from the object side to the image side. Surface and a second imaging surface. The first imaging plane is a specific visible light image plane perpendicular to the optical axis, and the central field of view has a maximum defocus modulation conversion contrast transfer rate (MTF) at the first spatial frequency; the second imaging plane is a specific vertical The defocus modulation conversion contrast transfer rate (MTF) of the infrared light image plane at the optical axis and its central field of view at the first spatial frequency has a maximum value. The first lens has a refractive power, and the object side may be a convex surface near the optical axis. The second lens has a refractive power. The third lens has a refractive power. The fourth lens has a refractive power. The fifth lens has a refractive power. The sixth lens has a refractive power. The seventh lens has a refractive power. The material of at least one of the first lens to the seventh lens is plastic and the material of at least one lens is glass. The optical imaging system is The image plane has a maximum imaging height HOI perpendicular to the optical axis, and at least one of the first lens to the seventh lens has a positive refractive power, and the focal lengths of the first lens to the seventh lens are f1, f2, respectively. f3, f4, f5, f6, f7, the focal length of the optical imaging system is f, the entrance pupil diameter of the optical imaging system is HEP, the distance from the object side of the first lens to the first imaging surface is HOS on the optical axis The half of the maximum viewing angle of the optical imaging system is HAF. The optical imaging system has a maximum imaging height HOI perpendicular to the optical axis on the first imaging plane. The first imaging plane and the second imaging plane are separated by light. The distance on the axis is FS. The intersection of any surface of any of these lenses with the optical axis is the starting point, and extends the contour of the surface until the vertical height of the surface at 1/2 of the entrance pupil diameter from the optical axis. Up to the coordinate point, the length of the contour curve between the two points is ARE, and the material of at least one of the first lens to the seventh lens is glass, which meets the following conditions: 1 ≦ f / HEP ≦ 10; 0deg <HAF ≦ 150deg; 1 ≦ 2 (ARE / HEP) ≦ 2.0 and | FS | 60μm.

According to the present invention, there is further provided an optical imaging system, which sequentially includes a first lens, a second lens, a third lens, a fourth lens, a fifth lens, a sixth lens, a seventh lens, and a first average from the object side to the image side. An imaging plane and a second average imaging plane. The first average imaging plane is a visible light image plane perpendicular to the optical axis and is arranged in the central field of view, the field of view of 0.3, and the field of view of 0.7 of the optical imaging system. Each of the first spatial frequencies has a maximum MTF of the field of view. The average position of the defocus position of the value; the second average imaging plane is a specific infrared light image plane perpendicular to the optical axis and is set in the central field of view, 0.3 field of view, and 0.7 field of view of the optical imaging system. The spatial frequencies all have an average position of the out-of-focus position of the maximum MTF value of the field of view. The optical imaging system has seven lenses with refractive power, the optical imaging system has a maximum imaging height HOI perpendicular to the optical axis on the first average imaging plane, and at least one of the first lens to the seventh lens The material of the lens is plastic and the material of at least one lens is glass. The first lens has a refractive power. The second lens has a refractive power. The third lens has a refractive power. The fourth lens has a refractive power. The fifth lens has a refractive power. The sixth lens has a refractive power. The seventh lens has a refractive power. And at least one of the first lens to the seventh lens has a positive refractive power, and the focal lengths of the first lens to the seventh lens are f1, f2, f3, f4, f5, f6, f7, and the optical imaging system. The entrance pupil diameter is HEP, the distance from the object side of the first lens to the first average imaging plane is HOS on the optical axis, half of the maximum viewing angle of the optical imaging system is HAF, and the optical imaging system is at the first The average imaging plane has a maximum imaging height HOI perpendicular to the optical axis. Any of these lenses The intersection point of any surface with the optical axis is the starting point, and extends the contour of the surface until the coordinate point on the surface at a vertical height of 1/2 of the entrance pupil diameter of the optical axis. The length of the contour curve between the two points is ARE , The distance between the first average imaging surface and the second average imaging surface is AFS, which satisfies the following conditions: 1 ≦ f / HEP ≦ 10; 0deg <HAF ≦ 150deg; 1 ≦ 2 (ARE / HEP) ≦ 2.0 and | AFS | ≦ 60 μm.

The length of the contour curve of any surface of a single lens within the maximum effective radius affects the surface's ability to correct aberrations and the optical path difference between rays of each field of view. The longer the length of the contour curve, the greater the ability to correct aberrations. It will increase the difficulty in production. Therefore, it is necessary to control the length of the contour curve within the maximum effective radius of any surface of a single lens, especially the length of the contour curve (ARS) and the surface within the maximum effective radius of the surface. The proportional relationship (ARS / TP) between the thickness (TP) of the lens on the optical axis. For example, the length of the contour curve of the maximum effective radius on the object side of the first lens is represented by ARS11, the thickness of the first lens on the optical axis is TP1, and the ratio between the two is ARS11 / TP1. The length of the contour curve is represented by ARS12, and the ratio between it and TP1 is ARS12 / TP1. The length of the contour curve of the maximum effective radius on the object side of the second lens is represented by ARS21, the thickness of the second lens on the optical axis is TP2, and the ratio between the two is ARS21 / TP2. The contour of the maximum effective radius of the image side of the second lens The length of the curve is represented by ARS22, and the ratio between it and TP2 is ARS22 / TP2. The proportional relationship between the length of the contour curve of the maximum effective radius of any of the surfaces of the remaining lenses in the optical imaging system and the thickness (TP) of the lens on the optical axis to which the surface belongs, and the expressions are deduced by analogy.

The infrared light has a wavelength between 700 nm and 1300 nm and the first spatial frequency is represented by SP1, which meets the following conditions: SP1 ≦ 440 cycles / mm.

The length of the contour curve of any surface of a single lens within the height range of 1/2 entrance pupil diameter (HEP) particularly affects the ability of the surface to correct aberrations in the common area of each ray field of view and the optical path difference between the fields of light. The longer the length of the contour curve, the better the ability to correct aberrations. However, it will also increase the difficulty of manufacturing. Therefore, it is necessary to control the contour of any surface of a single lens within the height of 1/2 incident pupil diameter (HEP). The length of the curve, especially the proportional relationship between the length of the contour curve (ARE) within the height of 1/2 of the entrance pupil diameter (HEP) of the surface and the thickness (TP) of the lens on the optical axis to which the surface belongs (ARE / TP). For example, the length of the contour curve of the 1/2 entrance pupil diameter (HEP) height of the first lens object side is represented by ARE11. The thickness of the first lens on the optical axis is TP1, and the ratio between the two is ARE11 / TP1, the length of the contour curve of the 1/2 entrance pupil diameter (HEP) height of the image side of the first lens is represented by ARE12, and the ratio between it and TP1 is ARE12 / TP1. The length of the profile curve of the 1/2 entrance pupil diameter (HEP) height of the second lens object side is represented by ARE21, the thickness of the second lens on the optical axis is TP2, and the ratio between the two is ARE21 / TP2. The profile curve length of the 1/2 entrance pupil diameter (HEP) height on the side is represented by ARE22, and the ratio between it and TP2 is ARE22 / TP2. The proportional relationship between the length of the contour curve of 1/2 of the entrance pupil diameter (HEP) height of any of the surfaces of the remaining lenses in the optical imaging system and the thickness (TP) of the lens on the optical axis to which the surface belongs. And so on.

When | f1 |> | f7 |, the total height of the optical imaging system (HOS; Height of Optic System) can be appropriately shortened to achieve the purpose of miniaturization.

At least one of the second lens to the sixth lens has a weak positive refractive power or a weak negative refractive power. The so-called weak refractive power means that the absolute value of the focal length of a particular lens is greater than 10mm. When at least one of the second to sixth lenses of the present invention has a weak positive refractive power, it can effectively share the positive refractive power of the first lens and prevent unnecessary aberrations from appearing prematurely. If at least one of the six lenses has a weak negative refractive power, the aberrations of the correction system can be fine-tuned.

In addition, the seventh lens may have a negative refractive power, and its image side may be concave. Thereby, it is advantageous to shorten the back focal length to maintain miniaturization. In addition, at least one surface of the seventh lens may have at least one inflection point, which can effectively suppress the incident angle of the off-axis field of view, and further correct the aberration of the off-axis field of view.

10, 20, 30, 40, 50, 60‧‧‧ optical imaging system

100, 200, 300, 400, 500, 600‧‧‧ aperture

110, 210, 310, 410, 510, 610‧‧‧ first lens

112, 212, 312, 412, 512, 612

114, 214, 314, 414, 514, 614‧‧‧ like side

120, 220, 320, 420, 520, 620‧‧‧ second lens

122, 222, 322, 422, 522, 622

124, 224, 324, 424, 524, 624‧‧‧ like side

130, 230, 330, 430, 530, 630‧‧‧ third lens

132, 232, 332, 432, 532, 632

134, 234, 334, 434, 534, 634 ‧ ‧ like side

140, 240, 340, 440, 540, 640‧‧‧ fourth lens

142, 242, 342, 442, 542, 642

144, 244, 344, 444, 544, 644‧‧‧ like side

150, 250, 350, 450, 550, 650‧‧‧ fifth lens

152, 252, 352, 452, 552, 652

154, 254, 354, 454, 554, 654‧‧‧ like side

160, 260, 360, 460, 560, 660‧‧‧ Sixth lens

162, 262, 362, 462, 562, 662

164, 264, 364, 464, 564, 664‧‧‧ like side

170, 270, 370, 470, 570, 670‧‧‧ seventh lens

172, 272, 372, 472, 572, 672

174, 274, 374, 474, 574, 674‧‧‧

180, 280, 380, 480, 580, 680‧‧‧ infrared filter

190, 290, 390, 490, 590, 690‧‧‧ first imaging plane

192, 292, 392, 492, 592, 692‧‧‧ image sensor

f‧‧‧ focal length of optical imaging system

f1‧‧‧ focal length of the first lens

f2‧‧‧ focal length of the second lens

f3‧‧‧ focal length of the third lens

f4‧‧‧ focal length of the fourth lens

f5‧‧‧ the focal length of the fifth lens

f6‧‧‧ focal length of the sixth lens

f7‧‧‧ focal length of the seventh lens

f / HEP; Fno; F # ‧‧‧ aperture value of optical imaging system

HAF‧‧‧half of the maximum viewing angle of optical imaging system

NA1‧‧‧The dispersion coefficient of the first lens

NA2, NA3, NA4, NA5, NA6, NA7‧The dispersion coefficient of the second lens to the seventh lens

R1, R2‧The curvature radius of the object side and the image side of the first lens

R3, R4‧The curvature radius of the object side and the image side of the second lens

R5, R6‧The curvature radius of the object side and image side of the third lens

R7, R8‧The curvature radius of the object side and image side of the fourth lens

R9, R10‧The curvature radius of the object side and image side of the fifth lens

R11, R12‧The curvature radius of the object side and image side of the sixth lens

R13, R14‧The curvature radius of the object side and image side of the seventh lens

TP1‧‧‧thickness of the first lens on the optical axis

TP2, TP3, TP4, TP5, TP6, TP7‧thickness of the second to seventh lenses on the optical axis

Σ TP‧‧‧ Total thickness of all refractive lenses

IN12‧‧‧ The distance between the first lens and the second lens on the optical axis

IN23‧‧‧ The distance between the second lens and the third lens on the optical axis

IN34‧‧‧ The distance between the third lens and the fourth lens on the optical axis

IN45‧‧‧ The distance between the fourth lens and the fifth lens on the optical axis

IN56‧‧‧The distance between the fifth lens and the sixth lens on the optical axis

IN67‧‧‧ The distance between the sixth lens and the seventh lens on the optical axis

InRS71‧‧‧ Horizontal displacement distance from the intersection of the seventh lens object side on the optical axis to the maximum effective radius position of the seventh lens object side on the optical axis

IF711‧‧‧The inflection point closest to the optical axis on the object side of the seventh lens

SGI711‧‧‧The amount of subsidence at this point

HIF711‧‧‧The vertical distance between the inflection point closest to the optical axis on the object side of the seventh lens and the optical axis

IF721‧‧‧The closest inflection point on the image side of the seventh lens closest to the optical axis

SGI721‧‧‧The amount of subsidence at this point

HIF721‧The vertical distance between the inflection point of the seventh lens image closest to the optical axis and the optical axis

IF712‧‧‧The second inflection point on the object side of the seventh lens near the optical axis

SGI712‧‧‧ Subsidence at this point

HIF712‧‧‧The vertical distance between the second curved point near the optical axis and the optical axis on the object side of the seventh lens

IF722‧‧‧The second inflection point on the image side of the seventh lens close to the optical axis

SGI722‧‧‧ Subsidence

HIF722‧‧‧ The vertical distance between the second curved point near the optical axis of the seventh lens image side and the optical axis

C71‧‧‧ critical point of the object side of the seventh lens

C72‧‧‧ critical point of the image side of the seventh lens

SGC71‧‧‧Horizontal displacement distance between the critical point of the object side of the seventh lens and the optical axis

SGC72‧The critical distance of the image side of the seventh lens and the horizontal displacement distance of the optical axis

HVT71‧‧‧The vertical distance between the critical point of the seventh lens and the optical axis

HVT72‧‧‧ The vertical distance between the critical point of the image side of the seventh lens and the optical axis

HOS‧‧‧ total system height (distance from the first lens object side to the first imaging plane on the optical axis)

InS‧‧‧ Distance from aperture to first imaging plane

InTL‧‧‧The distance from the object side of the first lens to the image side of the seventh lens

InB‧‧‧The distance from the image side of the seventh lens to the first imaging plane

HOI‧‧‧ half of the diagonal length of the effective sensing area of the image sensing element (maximum image height)

TDT‧‧‧TV Distortion of Optical Imaging System

ODT‧‧‧Optical Distortion of Optical Imaging System

The above and other features of the present invention will be described in detail with reference to the drawings.

FIG. 1A is a schematic diagram showing the optical imaging system of the first embodiment of the present invention; FIG. 1B is a diagram showing the spherical aberration, astigmatism, and optical distortion of the optical imaging system of the first embodiment of the present invention in order from left to right. Graph; FIG. 1C is a transverse aberration diagram of a meridional fan and a sagittal fan of the optical imaging system according to the first embodiment of the present invention, the longest working wavelength and the shortest working wavelength passing through the edge of the aperture at a field of view of 0.7; FIG. 1D is a diagram showing the center field of view, 0.3 field of view, and 0.7 field of view of the visible light spectrum in accordance with the first embodiment of the present invention. FIG. The central field of view, 0.3 field of view, and 0.7 field of view of the first embodiment of the defocus modulation conversion contrast transfer rate diagram; FIG. 2A is a schematic diagram showing the optical imaging system of the second embodiment of the present invention; Figure 2B shows the spherical aberration, astigmatism, and optical distortion of the optical imaging system of the second embodiment of the present invention in order from left to right. Figure 2C shows the meridian of the optical imaging system of the second embodiment of the present invention. Surface light fan and sagittal light fan, the longest working wavelength and the shortest working wavelength are transverse aberration diagrams at the 0.7 field of view through the edge of the aperture; the 2D diagram is the central field of view of the visible light spectrum of the second embodiment of the present invention, Defocus modulation conversion contrast transfer rate diagram for 0.3 field of view and 0.7 field of view; FIG. 2E is a diagram showing the central field of view, the field of view of 0.3, and the field of view of the second embodiment of the present invention. Comparative transfer rate chart; Figure 3A shows Schematic diagram of the optical imaging system of the third embodiment of the invention; FIG. 3B shows the spherical aberration, astigmatism, and optical distortion of the optical imaging system of the third embodiment of the invention in order from left to right; FIG. 3C A transverse aberration diagram of a meridional fan and a sagittal fan of the optical imaging system according to the third embodiment of the present invention, with the longest working wavelength and the shortest working wavelength passing through the aperture edge at a field of view of 0.7; FIG. 3D is a drawing The central field of view, visible field spectrum, 0.3 field of view, and 0.7 field of view of the third embodiment of the invention are compared with the defocus modulation conversion contrast transfer rate diagram; FIG. 3E is a diagram showing the central field of view of the infrared light spectrum of the third embodiment of the present invention Defocus modulation conversion vs. transfer rate chart for 0.3, 0.7 and 0.7 fields of view; FIG. 4A is a schematic diagram showing an optical imaging system according to a fourth embodiment of the present invention; FIG. 4B is a diagram showing spherical aberration, astigmatism, and optical distortion of the optical imaging system according to the fourth embodiment of the present invention in order from left to right. Graph; FIG. 4C is a transverse aberration diagram of a meridional fan and a sagittal fan of the fourth embodiment of the optical imaging system of the present invention, the longest working wavelength and the shortest working wavelength passing through the edge of the aperture at a field of view of 0.7; FIG. 4D is a diagram showing the defocus modulation conversion contrast transfer rate of the central field of view, 0.3 field of view, and 0.7 field of view of the visible light spectrum of the fourth embodiment of the present invention; FIG. 4E is a view of the fourth embodiment of the present invention Defocus modulation conversion contrast transfer rate diagram of the central field of view, 0.3 field of view, and 0.7 field of view of the infrared light spectrum; FIG. 5A is a schematic diagram showing the optical imaging system of the fifth embodiment of the present invention; FIG. 5B is from left to On the right, the spherical aberration, astigmatism, and optical distortion curves of the fifth embodiment of the optical imaging system of the present invention are plotted. Figure 5C shows the meridional light fans and arcs of the fifth embodiment of the optical imaging system of the present invention. Sagittal light fan, longest working The horizontal aberration diagram of the wavelength and the shortest working wavelength passing through the aperture edge at a field of view of 0.7; FIG. 5D is a diagram illustrating the central field of view, the field of view of 0.3, and the field of view of the defocus modulation of the visible light spectrum of the fifth embodiment of the present invention Conversion vs. transfer rate diagram; Figure 5E is a diagram showing the center-of-field, 0.3 field of view, and 0.7 field of view of the infrared light spectrum in accordance with the fifth embodiment of the present invention with defocus modulation conversion contrast transfer rate; Figure 6A is a diagram Schematic diagram of the optical imaging system of the sixth embodiment of the present invention; FIG. 6B shows the spherical aberration, astigmatism, and optical distortion of the optical imaging system of the sixth embodiment of the present invention in order from left to right; FIG. 6C Shows a meridional light fan and sagittal light of a sixth embodiment of the optical imaging system of the present invention. Fan, the longest working wavelength and the shortest working wavelength of the transverse aberration diagram at the 0.7 field of view through the edge of the aperture; Figure 6D shows the central field of view, 0.3 field of view, 0.7 field of view of the visible light spectrum of the sixth embodiment of the present invention FIG. 6E is a graph showing the defocus modulation conversion contrast transfer rate of the central field of view, 0.3 field of view, and 0.7 field of view of the infrared light spectrum of the sixth embodiment of the present invention.

An optical imaging system group includes a first lens, a second lens, a third lens, a fourth lens, a fifth lens, a sixth lens, a seventh lens, and a first lens having a refractive power in order from the object side to the image side. Imaging surface. The optical imaging system may further include an image sensing element disposed on the first imaging plane, and the imaging height approaches 3.91 mm in the following embodiments.

The optical imaging system can be designed using three working wavelengths, which are 486.1nm, 587.5nm, and 656.2nm, of which 587.5nm is the main reference wavelength and the reference wavelength for the main extraction technical features. The optical imaging system can also be designed using five working wavelengths, which are 470nm, 510nm, 555nm, 610nm, and 650nm, of which 555nm is the main reference wavelength and the reference wavelength for the main extraction technical features.

The ratio of the focal length f of the optical imaging system to the focal length fp of each lens with positive refractive power PPR, the ratio of the focal length f of the optical imaging system to the focal length fn of each lens with negative refractive power NPR, all lenses with positive refractive power The sum of PPR is Σ PPR, and the sum of NPR of all lenses with negative refractive power is Σ NPR. It helps to control the total refractive power and total length of the optical imaging system when the following conditions are met: 0.5 ≦ Σ PPR / | Σ NPR | ≦ 15. Preferably, the following conditions can be satisfied: 1 ≦ Σ PPR / | Σ NPR | ≦ 3.0.

The optical imaging system may further include an image sensing element disposed on the first imaging surface. The half of the diagonal length of the effective sensing area of the image sensing element (that is, the imaging height or maximum image height of the optical imaging system) is HOI, and the distance from the first lens object side to the first imaging surface on the optical axis is HOS , Which satisfies the following conditions: HOS / HOI ≦ 10; and 0.5 ≦ HOS / f ≦ 10. Preferably, the following conditions can be satisfied: 1 ≦ HOS / HOI ≦ 5; and 1 ≦ HOS / f ≦ 7. Thereby, the miniaturization of the optical imaging system can be maintained to be mounted on a thin and light portable electronic product.

In addition, in the optical imaging system of the present invention, at least one aperture can be set as required to reduce stray light and help improve image quality.

In the optical imaging system of the present invention, the aperture configuration may be a front aperture or a middle aperture, wherein the front aperture means that the aperture is set between the subject and the first lens, and the middle aperture means that the aperture is set between the first lens and the first lens. Between the first imaging planes. If the aperture is a front aperture, the exit pupil of the optical imaging system and the first imaging plane can have a longer distance to accommodate more optical elements, and increase the efficiency of the image sensing element to receive images; if the aperture is a middle aperture This system can help to expand the field of view of the system, so that the optical imaging system has the advantages of a wide-angle lens. The distance from the aforementioned aperture to the image side of the sixth lens is InS, which satisfies the following conditions: 0.2 ≦ InS / HOS ≦ 1.1. This makes it possible to achieve both the miniaturization of the optical imaging system and the characteristics of having a wide angle.

In the optical imaging system of the present invention, the distance between the object side of the first lens and the image side of the seventh lens is InTL, and the total thickness of all lenses with refractive power on the optical axis is Σ TP, which satisfies the following conditions: 0.1 ≦ Σ TP / InTL ≦ 0.9. Thereby, the contrast of the system imaging and the yield of lens manufacturing can be taken into account at the same time, and an appropriate back focus can be provided to accommodate other components.

The curvature radius of the object side of the first lens is R1, and the curvature radius of the image side of the first lens is R2, which satisfies the following conditions: 0.001 ≦ | R1 / R2 | ≦ 20. Thereby, the first lens has an appropriate positive refractive power strength, and avoids an increase in spherical aberration from overspeed. Preferably, the following conditions can be satisfied: 0.01 ≦ | R1 / R2 | <10.

The curvature radius of the object side of the seventh lens is R13, and the curvature radius of the image side of the seventh lens is R14, which satisfies the following conditions: -7 <(R11-R12) / (R11 + R12) <50. This is beneficial to correct the astigmatism generated by the optical imaging system.

The distance between the first lens and the second lens on the optical axis is IN12, which satisfies the following conditions: IN12 / f ≦ 3.0. This helps to improve the chromatic aberration of the lens to improve its performance.

The distance between the sixth lens and the seventh lens on the optical axis is IN67, which satisfies the following conditions: IN67 / f ≦ 0.8. This helps to improve the chromatic aberration of the lens to improve its performance.

The thicknesses of the first lens and the second lens on the optical axis are respectively TP1 and TP2, which satisfy the following conditions: 0.1 ≦ (TP1 + IN12) / TP2 ≦ 10. This helps to control the sensitivity of the optical imaging system manufacturing and improve its performance.

The thicknesses of the sixth lens and the seventh lens on the optical axis are TP6 and TP7, respectively. The distance between the two lenses on the optical axis is IN67, which satisfies the following conditions: 0.1 ≦ (TP7 + IN67) / TP6 ≦ 10. This helps to control the sensitivity of the optical imaging system manufacturing and reduce the overall system height.

The thicknesses of the third lens, the fourth lens, and the fifth lens on the optical axis are TP3, TP4, and TP5, respectively. The distance between the third lens and the fourth lens on the optical axis is IN34, and the fourth lens and the fifth lens are on the optical axis. The separation distance on the optical axis is IN45, and the distance from the object side of the first lens to the image side of the seventh lens is InTL, which satisfies the following conditions: 0.1 ≦ TP4 / (IN34 + TP4 + IN45) <1. This helps the layers to slightly correct the aberrations generated by the incident light and reduces the overall system height.

In the optical imaging system of the present invention, the vertical distance between the critical point C71 of the seventh lens object side and the optical axis is HVT71, the vertical distance of the critical point C72 of the seventh lens image side and the optical axis is HVT72, and the seventh lens object side is at The horizontal displacement distance from the intersection point on the optical axis to the critical point C71 on the optical axis is SGC71. The horizontal displacement distance from the intersection point on the optical axis of the seventh lens image side to the critical point C72 on the optical axis is SGC72, which can meet the following conditions. : 0mm ≦ HVT71 ≦ 3mm; 0mm <HVT72 ≦ 6mm; 0 ≦ HVT71 / HVT72; 0mm ≦ | SGC71 | ≦ 0.5mm; 0mm <| SGC72 | ≦ 2mm; and 0 <| SGC72 | / (| SGC72 | + TP7) ≦ 0.9. This can effectively correct aberrations in the off-axis field of view.

The optical imaging system of the present invention satisfies the following conditions: 0.2 ≦ HVT72 / HOI ≦ 0.9. Preferably, the following conditions can be satisfied: 0.3 ≦ HVT72 / HOI ≦ 0.8. This is helpful for aberration correction of the peripheral field of view of the optical imaging system.

The optical imaging system of the present invention satisfies the following conditions: 0 ≦ HVT72 / HOS ≦ 0.5. Preferably, the following conditions can be satisfied: 0.2 ≦ HVT72 / HOS ≦ 0.45. This is helpful for aberration correction of the peripheral field of view of the optical imaging system.

In the optical imaging system of the present invention, the horizontal displacement distance parallel to the optical axis between the intersection point of the seventh lens object side on the optical axis and the closest optical axis inflection point of the seventh lens object side is represented by SGI711. The seventh lens image The horizontal displacement distance parallel to the optical axis between the intersection of the side on the optical axis and the closest optical axis of the seventh lens image side is expressed as SGI721, which satisfies the following conditions: 0 <SGI711 / (SGI711 + TP7) ≦ 0.9 ; 0 <SGI721 / (SGI721 + TP7) ≦ 0.9. Preferably, the following conditions can be satisfied: 0.1 ≦ SGI711 / (SGI711 + TP7) ≦ 0.6; 0.1 ≦ SGI721 / (SGI721 + TP7) ≦ 0.6.

The horizontal displacement distance parallel to the optical axis between the intersection of the seventh lens object side on the optical axis and the second curved point near the optical axis of the seventh lens object side is represented by SGI712. The horizontal displacement distance parallel to the optical axis between the intersection point and the second curved optical axis of the seventh lens image side parallel to the optical axis is represented by SGI722, which satisfies the following conditions: 0 <SGI712 / (SGI712 + TP7) ≦ 0.9; 0 <SGI722 / (SGI722 + TP7) ≦ 0.9. Preferably, the following conditions can be satisfied: 0.1 ≦ SGI712 / (SGI712 + TP7) ≦ 0.6; 0.1 ≦ SGI722 / (SGI722 + TP7) ≦ 0.6.

The vertical distance between the inflection point of the closest optical axis of the seventh lens object side and the optical axis is represented by HIF711. The intersection of the seventh lens image side on the optical axis to the closest optical axis of the seventh lens image side and the inflection point of the optical axis The vertical distance between them is represented by HIF721, which satisfies the following conditions: 0.001mm ≦ | HIF711 | ≦ 5mm; 0.001mm ≦ | HIF721 | ≦ 5mm. Preferably, the following conditions can be satisfied: 0.1mm ≦ | HIF711 | ≦ 3.5mm; 1.5mm ≦ | HIF721 | ≦ 3.5mm.

The vertical distance between the second curved point near the optical axis of the seventh lens object side and the optical axis is represented by HIF712. The intersection of the seventh lens image side on the optical axis to the seventh lens image side second curve near the optical axis The vertical distance between the point and the optical axis is represented by HIF722, which satisfies the following conditions: 0.001mm ≦ | HIF712 | ≦ 5mm; 0.001mm ≦ | HIF722 | ≦ 5mm. Preferably, the following conditions can be satisfied: 0.1mm ≦ | HIF722 | ≦ 3.5mm; 0.1mm ≦ | HIF712 | ≦ 3.5mm.

The vertical distance between the inflection point of the seventh lens object side close to the optical axis and the optical axis is represented by HIF713. The intersection of the seventh lens image side on the optical axis and the seventh lens image side is the third curve close to the optical axis. The vertical distance between the point and the optical axis is represented by HIF723, which satisfies the following conditions: 0.001mm ≦ | HIF713 | ≦ 5mm; 0.001mm ≦ | HIF723 | ≦ 5mm. Preferably, the following conditions can be satisfied: 0.1mm ≦ | HIF723 | ≦ 3.5mm; 0.1mm ≦ | HIF713 | ≦ 3.5mm.

The vertical distance between the inflection point of the seventh lens object side close to the optical axis and the optical axis is represented by HIF714. The intersection of the seventh lens image side on the optical axis to the seventh lens image side is the fourth curve close to the optical axis. The vertical distance between the point and the optical axis is represented by HIF724, which satisfies the following conditions: 0.001mm ≦ | HIF714 | ≦ 5mm; 0.001mm ≦ | HIF724 | ≦ 5mm. Preferably, the following conditions can be satisfied: 0.1mm ≦ | HIF724 | ≦ 3.5mm; 0.1mm ≦ | HIF714 | ≦ 3.5mm.

According to an embodiment of the optical imaging system of the present invention, the lenses with high dispersion coefficient and low dispersion coefficient can be staggered to help correct the chromatic aberration of the optical imaging system.

The equation of the above aspheric surface is: z = ch ² / [1+ [l- (k + 1) c ² h ² ] 0.5] + A4h ⁴ + A6h ⁶ + A8h ⁸ + A10h ¹⁰ + A12h ¹² + A14h ¹⁴ + A16h ¹⁶ + A18h ¹⁸ + A20h ²⁰ +… (1) where z is the position value with the surface vertex as the reference at the position of height h along the optical axis direction, k is the cone coefficient, c is the inverse of the radius of curvature, and A4, A6, A8, A10, A12, A14, A16, A18 and A20 are high-order aspheric coefficients.

In the optical imaging system provided by the present invention, the material of the lens may be plastic or glass. When the lens is made of plastic, it can effectively reduce production costs and weight. In addition, when the material of the lens is glass, the thermal effect can be controlled and the design space of the refractive power configuration of the optical imaging system can be increased. In addition, the object side and the image side of the first to seventh lenses in the optical imaging system can be aspheric, which can obtain more control variables. In addition to reducing aberrations, compared with the use of traditional glass lenses, The number of lenses used can be reduced, so the overall height of the optical imaging system of the present invention can be effectively reduced.

Furthermore, in the optical imaging system provided by the present invention, if the lens surface is convex, in principle, the lens surface is convex at the near optical axis; if the lens surface is concave, in principle, the lens surface is at the near optical axis. Concave.

The optical imaging system of the present invention can be applied to an optical system for mobile focusing as required, and has both the characteristics of excellent aberration correction and good imaging quality, thereby expanding the application level.

The optical imaging system of the present invention may further include a driving module as required. The driving module may be coupled to the lenses and cause the lenses to be displaced. The aforementioned driving module may be a voice coil motor (VCM) for driving the lens to focus, or an optical anti-shake element (OIS) for reducing the frequency of out-of-focus caused by lens vibration during shooting.

According to the optical imaging system of the present invention, at least one of the first lens, the second lens, the third lens, the fourth lens, the fifth lens, the sixth lens, and the seventh lens may be a light filtering element with a wavelength less than 500 nm according to the needs. It can be achieved by coating on at least one surface of the specific lens with a filtering function or the lens itself is made of a material with a filterable short wavelength.

The first imaging surface of the optical imaging system of the present invention may be selected as a plane or a curved surface as required. When the first imaging surface is a curved surface (such as a spherical surface with a radius of curvature), it is helpful to reduce the incident angle required to focus the light on the first imaging surface. In addition to helping to achieve the length of the miniature optical imaging system (TTL) , And also help to improve the contrast.

According to the foregoing implementation manners, specific examples are provided below and described in detail with reference to the drawings.

First embodiment

Please refer to FIG. 1A and FIG. 1B, wherein FIG. 1A shows a schematic diagram of an optical imaging system according to the first embodiment of the present invention, and FIG. 1B shows the optical imaging system of the first embodiment in order from left to right. Spherical aberration, astigmatism and optical distortion curves. FIG. 1C is a meridional light fan and a sagittal light fan of the optical imaging system of the first embodiment. The longest working wavelength and the shortest working wavelength pass through. Lateral aberration diagram at the aperture edge at 0.7 field of view. FIG. 1D is a diagram showing the center-of-view, 0.3-field, and 0.7-field defocus modulation conversion contrast transfer rate diagrams of the visible light spectrum according to the embodiment of the present invention; FIG. 1E is a first focus of the present invention. Defocus modulation conversion vs. transfer rate diagram for the central field of view, 0.3 field of view, and 0.7 field of view of the infrared light spectrum of the embodiment. As can be seen from FIG. 1A, the optical imaging system includes a first lens 110, an aperture 100, a second lens 120, a third lens 130, a fourth lens 140, a fifth lens 150, and a sixth lens 160 in this order from the object side to the image side. And a seventh lens 170, an infrared filter 180, a first imaging surface 190, and an image sensing element 192.

The first lens 110 has a negative refractive power and is made of plastic. Its object side 112 is concave, its image side 114 is concave and both are aspheric, and its object side 112 has an inflection point and the image side 114 has two Inflection point. The length of the contour curve of the maximum effective radius on the object side of the first lens is represented by ARS11, and the length of the contour curve of the maximum effective radius of the image side of the first lens is represented by ARS12. The length of the contour curve of the 1/2 incident pupil diameter (HEP) on the object side of the first lens is represented by ARE11, and the length of the contour curve of the 1/2 incidence pupil diameter (HEP) of the first lens image side is represented by ARE12. The thickness of the first lens on the optical axis is TP1.

The horizontal displacement distance parallel to the optical axis between the intersection of the object side of the first lens on the optical axis and the closest optical axis inflection point of the object side of the first lens is represented by SGI111. The intersection of the image side of the first lens on the optical axis to The horizontal displacement distance between the inflection points of the closest optical axis of the first lens image side parallel to the optical axis is represented by SGI121, which satisfies the following conditions: SGI111 = -0.1110mm; SGI121 = 2.7120mm; TP1 = 2.2761mm; | SGI111 | /(|SGI111|+TP1)=0.0465; | SGI121 | / (| SGI121 | + TP1) = 0.5437.

The horizontal displacement distance parallel to the optical axis between the intersection point of the first lens image side on the optical axis and the second curved point close to the optical axis of the first lens image side is represented by SGI122, which satisfies the following conditions: SGI122 = 4.2315mm; | SGI122 | / (| SGI122 | + TP1) = 0.6502.

The vertical distance between the inflection point of the closest optical axis of the object side of the first lens and the optical axis is represented by HIF111. The intersection point of the first lens image side on the optical axis to the inflection point of the closest optical axis of the first lens image side and the optical axis The vertical distance between them is represented by HIF121, which meets the following conditions: HIF111 = 12.8432mm; HIF111 / HOI = 1.7127; HIF121 = 7.1744mm; HIF121 / HOI = 0.9567.

The vertical distance between the point of intersection of the first lens image side on the optical axis and the second lens image side closest to the inflection point closest to the optical axis and the optical axis is represented by HIF122, which satisfies the following conditions: HIF122 = 9.8592mm; HIF122 / HOI = 1.3147.

The second lens 120 has a positive refractive power and is made of plastic. The object side surface 122 is a convex surface, and the image side surface 124 is a concave surface. The length of the contour curve of the maximum effective radius on the object side of the second lens is represented by ARS21, and the length of the contour curve of the maximum effective radius of the image side of the second lens is represented by ARS22. The length of the profile curve of 1/2 incident pupil diameter (HEP) on the object side of the second lens is represented by ARE21, and the length of the profile curve of 1/2 incident pupil diameter (HEP) on the image side of the second lens is represented by ARE22. The thickness of the second lens on the optical axis is TP2.

The horizontal displacement distance parallel to the optical axis between the intersection point of the second lens object side on the optical axis and the closest optical axis inflection point of the second lens object side is represented by SGI211. The intersection point of the second lens image side on the optical axis is The horizontal displacement distance between the inflection points of the closest optical axis of the second lens image side parallel to the optical axis is represented by SGI221.

The vertical distance between the inflection point of the closest optical axis of the second lens object side and the optical axis is represented by HIF211. The intersection of the second lens image side on the optical axis to the closest optical axis of the second lens image side and the inflection point of the optical axis The vertical distance between them is indicated by HIF221.

The third lens 130 has a negative refractive power and is made of plastic material. Its object side surface 132 is convex, its image side surface 134 is concave, and all of them are aspheric. The length of the contour curve of the maximum effective radius on the object side of the third lens is represented by ARS31, and the length of the contour curve of the maximum effective radius of the image side of the third lens is represented by ARS32. The length of the contour curve of 1/2 incident pupil diameter (HEP) on the object side of the third lens is represented by ARE31, and the length of the contour curve of 1/2 incident pupil diameter (HEP) on the image side of the third lens is represented by ARE32. The thickness of the third lens on the optical axis is TP3.

The horizontal displacement distance parallel to the optical axis between the intersection point of the third lens object side on the optical axis and the closest optical axis inflection point of the third lens object side is represented by SGI311. The intersection point of the third lens image side on the optical axis is The horizontal displacement distance between the inflection points of the closest optical axis of the third lens image side parallel to the optical axis is represented by SGI321.

The horizontal displacement distance parallel to the optical axis between the intersection of the object side of the third lens on the optical axis and the second inflection point of the object side of the third lens close to the optical axis is represented by SGI312. The image side of the third lens on the optical axis The horizontal displacement distance from the intersection point to the inflection point of the third lens image side close to the optical axis parallel to the optical axis is represented by SGI322.

The vertical distance between the inflection point of the closest optical axis of the third lens object side and the optical axis is represented by HIF311. The intersection of the third lens image side on the optical axis to the closest optical axis of the third lens image side and the inflection point of the optical axis The vertical distance between them is indicated by HIF321.

The vertical distance between the second inflection point of the third lens object side close to the optical axis and the optical axis is represented by HIF312. The intersection of the third lens image side on the optical axis to the second lens image side second inflection near the optical axis The vertical distance between the point and the optical axis is represented by HIF322.

The fourth lens 140 has a positive refractive power and is made of a plastic material. Its object side surface 142 is convex, its image side surface 144 is convex, and both are aspheric. The object side surface 142 has an inflection point. The length of the contour curve of the maximum effective radius on the object side of the fourth lens is represented by ARS41, and the length of the contour curve of the maximum effective radius of the image side of the fourth lens is represented by ARS42. The length of the contour curve of the 1/2 incident pupil diameter (HEP) on the object side of the fourth lens is represented by ARE41, and the length of the contour curve of the 1/2 incidence pupil diameter (HEP) of the fourth lens image side is represented by ARE42. The thickness of the fourth lens on the optical axis is TP4.

The horizontal displacement distance parallel to the optical axis between the intersection point of the fourth lens object side on the optical axis and the closest optical axis inflection point of the fourth lens object side is represented by SGI411. The intersection point of the fourth lens image side on the optical axis is The horizontal displacement distance between the inflection points of the closest optical axis of the fourth lens image side parallel to the optical axis is represented by SGI421, which satisfies the following conditions: SGI411 = 0.0018mm; | SGI411 | / (| SGI411 | + TP4) = 0.0009.

The horizontal displacement distance parallel to the optical axis between the intersection of the object side of the fourth lens on the optical axis and the second inflection point of the object side of the fourth lens close to the optical axis is represented by SGI412. The image side of the fourth lens on the optical axis The horizontal displacement distance parallel to the optical axis between the intersection point and the inflection point of the fourth lens image side close to the optical axis is represented by SGI422.

The vertical distance between the inflection point of the closest optical axis of the fourth lens object side and the optical axis is represented by HIF411. The intersection point of the fourth lens image side on the optical axis to the closest optical axis of the fourth lens image side and the inflection point of the optical axis The vertical distance between them is represented by HIF421, which meets the following conditions: HIF411 = 0.7191mm; HIF411 / HOI = 0.0959.

The vertical distance between the second inflection point of the fourth lens object side close to the optical axis and the optical axis is represented by HIF412. The intersection of the fourth lens image side on the optical axis to the second lens image side second inflection near the optical axis The vertical distance between the point and the optical axis is represented by HIF422.

The fifth lens 150 has a positive refractive power and is made of plastic. The object side surface 152 is concave, the image side 154 is convex, and both are aspheric. The object side 152 and the image side 154 each have an inflection point. The length of the contour curve of the maximum effective radius on the object side of the fifth lens is represented by ARS51, and the length of the contour curve of the maximum effective radius of the image side of the fifth lens is represented by ARS52. The length of the contour curve of the 1/2 incident pupil diameter (HEP) on the object side of the fifth lens is represented by ARE51, and the image side of the fifth lens The length of the contour curve of 1/2 of the entrance pupil diameter (HEP) is represented by ARE52. The thickness of the fifth lens on the optical axis is TP5.

The horizontal displacement distance parallel to the optical axis between the intersection of the fifth lens's object side on the optical axis and the closest optical axis's inflection point on the fifth lens's object side is represented by SGI511. The intersection of the fifth lens's image side on the optical axis to The horizontal displacement distance between the inflection points of the closest optical axis of the fifth lens image side parallel to the optical axis is represented by SGI521, which satisfies the following conditions: SGI511 = -0.1246mm; SGI521 = -2.1477mm; | SGI511 | / (| SGI511 | + TP5) = 0.0284; | SGI521 | / (| SGI521 | + TP5) = 0.3346.

The horizontal displacement distance parallel to the optical axis between the intersection point of the fifth lens object side on the optical axis and the second inflection point of the fifth lens object side close to the optical axis is represented by SGI512. The horizontal displacement distance parallel to the optical axis between the intersection point and the inflection point of the fifth lens image side close to the optical axis is represented by SGI522.

The vertical distance between the inflection point of the closest optical axis on the object side of the fifth lens and the optical axis is represented by HIF511, and the vertical distance between the inflection point of the closest optical axis on the side of the fifth lens image and the optical axis is represented by HIF521. : HIF511 = 3.8179mm; HIF521 = 4.5480mm; HIF511 / HOI = 0.5091; HIF521 / HOI = 0.6065.

The vertical distance between the second inflection point of the fifth lens surface close to the optical axis and the optical axis is represented by HIF512, and the vertical distance between the second inflection point of the fifth lens image side close to the optical axis and the optical axis is HIF522.

The sixth lens 160 has a negative refractive power and is made of plastic material. Its object side surface 162 is convex, its image side 164 is concave, and both its object side 162 and image side 164 have an inflection point. This can effectively adjust the angle of incidence of each field of view on the sixth lens to improve aberrations. The length of the contour curve of the maximum effective radius on the object side of the sixth lens is represented by ARS61, and the length of the contour curve of the maximum effective radius of the image side of the sixth lens is represented by ARS62. The length of the contour curve of the 1/2 incident pupil diameter (HEP) on the object side of the sixth lens is represented by ARE61, and the length of the contour curve of the 1/2 incidence pupil diameter (HEP) of the sixth lens image side is represented by ARE62. The thickness of the sixth lens on the optical axis is TP6.

The horizontal displacement distance parallel to the optical axis between the intersection point of the sixth lens object side on the optical axis and the closest optical axis inflection point of the sixth lens object side is represented by SGI611. The intersection point of the sixth lens image side on the optical axis is The horizontal displacement distance between the inflection points of the closest optical axis of the sixth lens image side parallel to the optical axis is represented by SGI621, which satisfies the following conditions: SGI611 = 0.3208mm; SGI621 = 0.5937 mm; | SGI611 | / (| SGI611 | + TP6) = 0.5167; | SGI621 | / (| SGI621 | + TP6) = 0.6643.

The vertical distance between the inflection point of the closest optical axis on the object side of the sixth lens and the optical axis is represented by HIF611, and the vertical distance between the inflection point of the closest optical axis on the side of the sixth lens image and the optical axis is represented by HIF621, which meets the following conditions : HIF611 = 1.9655mm; HIF621 = 2.0041mm; HIF611 / HOI = 0.2621; HIF621 / HOI = 0.2672.

The seventh lens 170 has a positive refractive power and is made of plastic. The object side surface 172 is a convex surface and the image side surface 174 is a concave surface. Thereby, it is advantageous to shorten the back focal length to maintain miniaturization. In addition, each of the object side surface 172 and the image side surface 174 has an inflection point. The length of the contour curve of the maximum effective radius on the object side of the seventh lens is represented by ARS71, and the length of the contour curve of the maximum effective radius of the image side of the seventh lens is represented by ARS72. The length of the contour curve of 1/2 incident pupil diameter (HEP) on the object side of the seventh lens is represented by ARE71, and the length of the contour curve of 1/2 incident pupil diameter (HEP) on the image side of the seventh lens is represented by ARE72. The thickness of the seventh lens on the optical axis is TP7.

The horizontal displacement distance parallel to the optical axis between the intersection point of the seventh lens object side on the optical axis and the closest optical axis inflection point of the seventh lens object side is represented by SGI711. The intersection point of the seventh lens image side on the optical axis is The horizontal displacement distance between the inflection points of the closest optical axis of the seventh lens image side parallel to the optical axis is represented by SGI721, which satisfies the following conditions: SGI711 = 0.5212mm; SGI721 = 0.5668mm; | SGI711 | / (| SGI711 | + TP7) = 0.3179; | SGI721 | / (| SGI721 | + TP7) = 0.3364.

The vertical distance between the inflection point of the closest optical axis on the object side of the seventh lens and the optical axis is represented by HIF711, and the vertical distance between the inflection point of the closest optical axis on the image side of the seventh lens and the optical axis is represented by HIF721, which satisfies the following conditions : HIF711 = 1.6707mm; HIF721 = 1.8616mm; HIF711 / HOI = 0.2228; HIF721 / HOI = 0.2482.

The features described below in this embodiment and the inflection point are obtained based on the main reference wavelength of 555 nm.

The infrared filter 180 is made of glass and is disposed between the seventh lens 170 and the first imaging surface 190 without affecting the focal length of the optical imaging system.

In the optical imaging system of this embodiment, the focal length of the optical imaging system is f, the entrance pupil diameter of the optical imaging system is HEP, and the half of the maximum viewing angle in the optical imaging system is HAF, and the value is as follows: f = 4.3019mm; f / HEP = 1.2; and HAF = 59.9968 degrees and tan (HAF) = 1.7318.

In the optical imaging system of this embodiment, the focal length of the first lens 110 is f1, and the focal length of the seventh lens 170 is f7, which satisfies the following conditions: f1 = -14.5286mm; | f / f1 | = 0.2961; f7 = 8.2933mm ; | F1 |> f7; and | f1 / f7 | = 1.7519.

In the optical imaging system of this embodiment, the focal lengths of the second lens 120 to the sixth lens 160 are f2, f3, f4, f5, and f6, respectively, which satisfy the following conditions: | f2 | + | f3 | + | f4 | + | f5 | + | f6 | = 144.7494mm; | f1 | + | f7 | = 22.8219mm and | f2 | + | f3 | + | f4 | + | f5 | + | f6 |> | f1 | + | f7 |.

The ratio of the focal length f of the optical imaging system to the focal length fp of each lens with a positive refractive power, PPR, and the ratio of the focal length f of the optical imaging system to the focal length fn of each lens with a negative refractive power, NPR. The optical imaging of this embodiment In the system, the sum of PPR of all positive refractive lenses is Σ PPR = f / f2 + f / f4 + f / f5 + f / f7 = 1.7384, and the sum of NPR of all negative refractive lenses is Σ NPR = f / f1 + f / f3 + f / f6 = -0.9999, Σ PPR / | Σ NPR | = 1.7386. The following conditions are also met: | f / f2 | = 0.1774; | f / f3 | = 0.0443; | f / f4 | = 0.4411; | f / f5 | = 0.6012; | f / f6 | = 0.6595; | f / f7 | = 0.5187.

In the optical imaging system of this embodiment, the distance between the first lens object side 112 to the seventh lens image side 174 is InTL, the distance between the first lens object side 112 to the first imaging surface 190 is HOS, and the aperture 100 to the first The distance between an imaging surface 190 is InS, half of the diagonal length of the effective sensing area of the image sensing element 192 is HOI, and the distance from the image side 174 of the seventh lens to the first imaging surface 190 is BFL, which meets the following conditions : InTL + BFL = HOS; HOS = 26.9789mm; HOI = 7.5mm; HOS / HOI = 3.5977; HOS / f = 6.2715; InS = 12.4615mm; and InS / HOS = 0.4619.

In the optical imaging system of this embodiment, the sum of the thicknesses of all the lenses with refractive power on the optical axis is Σ TP, which satisfies the following conditions: Σ TP = 16.0446mm; and Σ TP / InTL = 0.6559. Thereby, the contrast of the system imaging and the yield of lens manufacturing can be taken into account at the same time, and an appropriate back focus can be provided to accommodate other components.

In the optical imaging system of this embodiment, the curvature radius of the object side 112 of the first lens is R1, and the curvature radius of the image side 114 of the first lens is R2, which satisfies the following conditions: | R1 / R2 | = 129.9952. Thereby, the first lens has an appropriate positive refractive power strength, and avoids an increase in spherical aberration from overspeed.

In the optical imaging system of this embodiment, the curvature radius of the object side surface 172 of the seventh lens Is R13, and the curvature radius of the image side 174 of the seventh lens is R14, which satisfies the following conditions: (R13-R14) / (R13 + R14) =-0.0806. This is beneficial to correct the astigmatism generated by the optical imaging system.

In the optical imaging system of this embodiment, the sum of the focal lengths of all lenses with positive refractive power is Σ PP, which satisfies the following conditions: Σ PP = f2 + f4 + f5 + f7 = 49.4535mm; and f4 / (f2 + f4 + f5 + f7) = 0.1972. Therefore, it is helpful to appropriately allocate the positive refractive power of the fourth lens 140 to other positive lenses, so as to suppress the occurrence of significant aberrations during the traveling process of incident light.

In the optical imaging system of this embodiment, the sum of the focal lengths of all lenses with negative refractive power is Σ NP, which satisfies the following conditions: Σ NP = f1 + f3 + f6 = -118.1178mm; and f1 / (f1 + f3 + f6 ) = 0.1677. Therefore, it is helpful to appropriately allocate the negative refractive power of the first lens to other negative lenses, so as to suppress the occurrence of significant aberrations during the traveling process of incident light.

In the optical imaging system of this embodiment, the distance between the first lens 110 and the second lens 120 on the optical axis is IN12, which satisfies the following conditions: IN12 = 4.5524mm; IN12 / f = 1.0582. This helps to improve the chromatic aberration of the lens to improve its performance.

In the optical imaging system of this embodiment, the thicknesses of the first lens 110 and the second lens 120 on the optical axis are TP1 and TP2, respectively, which satisfy the following conditions: TP1 = 2.2761mm; TP2 = 0.2398mm; and (TP1 + IN12 ) /TP2=1.3032. This helps to control the sensitivity of the optical imaging system manufacturing and improve its performance.

In the optical imaging system of this embodiment, the thicknesses of the sixth lens 160 and the seventh lens 170 on the optical axis are TP6 and TP7, respectively. The distance between the two lenses on the optical axis is IN67, which meets the following conditions: TP6 = 0.3000mm; TP7 = 1.1182mm; and (TP7 + IN67) /TP6=4.4322. This helps to control the sensitivity of the optical imaging system manufacturing and reduce the overall system height.

In the optical imaging system of this embodiment, the thicknesses of the third lens 130, the fourth lens 140, and the fifth lens 150 on the optical axis are TP3, TP4, and TP5, respectively. The third lens 130 and the fourth lens 140 are on the optical axis. The separation distance of the lens is IN34, the separation distance of the fourth lens 140 and the fifth lens 150 on the optical axis is IN45, and the distance between the object side 112 of the first lens and the image side 174 of the seventh lens is InTL, which meets the following conditions: TP3 = 0.8369mm; TP4 = 2.0022mm; TP5 = 4.2706mm; IN34 = 1.9268mm; IN45 = 1.5153mm; and TP4 / (IN34 + TP4 + IN45) = 0.3678. This helps to correct the aberrations produced by the incident light and to reduce the total height of the system.

In the optical imaging system of this embodiment, the horizontal displacement distance from the intersection of the sixth lens object side 162 on the optical axis to the maximum effective radius position of the sixth lens object side 162 on the optical axis is InRS61, and the sixth lens image side 164 is on The horizontal displacement distance from the intersection point on the optical axis to the maximum effective radius position of the sixth lens image side 164 on the optical axis is InRS62, and the thickness of the sixth lens 160 on the optical axis is TP6, which meets the following conditions: InRS61 = -0.7823mm ; InRS62 = -0.2166mm; and | InRS62 | /TP6=0.722. This helps to make and shape the lens, and effectively maintains its miniaturization.

In the optical imaging system of this embodiment, the vertical distance between the critical point of the sixth lens object side surface 162 and the optical axis is HVT61, and the vertical distance between the critical point of the sixth lens image side 164 and the optical axis is HVT62, which meets the following conditions: HVT61 = 3.3498mm; HVT62 = 3.9860mm; and HVT61 / HVT62 = 0.8404.

In the optical imaging system of this embodiment, the horizontal displacement distance from the intersection of the seventh lens object side 172 on the optical axis to the maximum effective radius position of the seventh lens object side 172 on the optical axis is InRS71, and the seventh lens image side 174 is on The horizontal displacement distance from the intersection point on the optical axis to the maximum effective radius position of the seventh lens image side 174 on the optical axis is InRS72. The thickness of the seventh lens 170 on the optical axis is TP7, which meets the following conditions: InRS71 = -0.2756mm ; InRS72 = -0.0938mm; and | InRS72 | /TP7=0.0839. This helps to make and shape the lens, and effectively maintains its miniaturization.

In the optical imaging system of this embodiment, the vertical distance between the critical point of the seventh lens object side 172 and the optical axis is HVT71, and the vertical distance between the critical point of the seventh lens image side 174 and the optical axis is HVT72, which satisfies the following conditions: HVT71 = 3.6822mm; HVT72 = 4.0606mm; and HVT71 / HVT72 = 0.9068. This can effectively correct aberrations in the off-axis field of view.

In the optical imaging system of this embodiment, it satisfies the following conditions: HVT72 / HOI = 0.5414. This is helpful for aberration correction of the peripheral field of view of the optical imaging system.

In the optical imaging system of this embodiment, it satisfies the following conditions: HVT72 / HOS = 0.1505. This is helpful for aberration correction of the peripheral field of view of the optical imaging system.

In the optical imaging system of this embodiment, the second lens, the third lens, and the seventh lens have negative refractive power, the dispersion coefficient of the second lens is NA2, the dispersion coefficient of the third lens is NA3, and the dispersion coefficient of the seventh lens is NA7, which satisfies the following conditions: 1 ≦ NA7 / NA2. This helps to correct the chromatic aberration of the optical imaging system.

In the optical imaging system of this embodiment, the TV distortion of the optical imaging system during the image formation is TDT and the optical distortion during the image formation is ODT, which satisfies the following conditions: | TDT | = 2.5678%; | ODT | = 2.1302%.

The light in any field of view of the embodiment of the present invention can be further divided into sagittal ray and tangential ray, and the evaluation basis of the focus offset and MTF value is a spatial frequency of 110 cycles / mm. The focus offsets of the maximum defocus MTF of the sagittal rays of the central field of view, 0.3 fields of view, and 0.7 fields of view are represented by VSFS0, VSFS3, and VSFS7 (measurement units: mm), and the values are 0.000mm,- 0.005mm, 0.000mm; the maximum value of the defocus MTF of the sagittal rays of the central field of view, 0.3 field of view, and 0.7 field of view is represented by VSMTF0, VSMTF3, and VSMTF7, and the values are 0.886, 0.885, and 0.863; The focus offsets of the maximum defocus MTF of the meridional rays in the field, 0.3 field of view, and 0.7 field of view are represented by VTFS0, VTFS3, and VTFS7 (measurement units: mm), and the values are 0.000mm, 0.001mm,- 0.005mm; the maximum defocus MTF of the meridional rays in the central field of view, 0.3 field of view, and 0.7 field of view are represented by VTMTF0, VTMTF3, and VTMTF7, and the values are 0.886, 0.868, and 0.796, respectively. The average focus shift amount (position) of the focus shift amounts of the aforementioned sagittal three-view field of the visible arc and the meridional three-view field of visible light is represented by AVFS (unit of measurement: mm), which satisfies the absolute value VTFS0 + VTFS3 + VTFS7) / 6 | = | 0.000mm |.

In this embodiment, the focus offsets of the maximum defocus MTF of the sagittal rays of the central field of view, the field of view of 0.3, and the field of view of 0.7 are represented by ISFS0, ISFS3, and ISFS7 (unit of measurement: mm), and the values are respectively It is 0.025mm, 0.020mm, 0.020mm. The average focus offset (position) of the aforementioned three focus fields of the sagittal plane is represented by AISFS; the center of the infrared light field, the 0.3 field of view, and the sagittal plane of the 0.7 field of view The maximum defocus MTF of the light is represented by ISMTF0, ISMTF3, and ISMTF7, and the values are 0.787, 0.802, and 0.772 respectively; the maximum defocus MTF of the meridional rays of the central field, 0.3 field, and 0.7 field of infrared light The focus offsets are respectively represented by ITFS0, ITFS3, and ITFS7 (units of measurement: mm), and their values are 0.025, 0.035, and 0.035, respectively. The average focus offset (position) of the focus offsets of the three fields of view of the meridian plane is AITFS (measurement unit: mm); the maximum defocus MTF of the meridional rays of the central field of view, 0.3 field of view, and 0.7 field of view of the infrared light is represented by IMTTF0, IMTTF3, and IMTTF7, and the values are 0.787, 0.805, 0.721, respectively . The average focus offset (position) of the aforementioned infrared light sagittal three-field and infrared light meridional three-field is represented by AIFS (measurement unit: mm), which satisfies the absolute value | (ISFS0 + ISFS3 + ISFS7 + ITFS0 + ITFS3 + ITFS7) / 6 | = | 0.02667mm |.

The focus offset between the visible light center field focus point and the infrared light center field focus point (RGB / IR) of the entire optical imaging system in this embodiment is represented by FS (that is, a wavelength of 850 nm to a wavelength of 555 nm, a unit of measurement: mm) , Which satisfies the absolute value | (VSFS0 + VTFS0) / 2- (ISFS0 + ITFS0) / 2 | = | 0.025mm |; the average focus offset of the visible light three field of view and the average focus of the three field of infrared light of the entire optical imaging system The difference between the offsets (RGB / IR) (focus offset) is expressed in AFS (that is, a wavelength of 850 nm to a wavelength of 555 nm, a unit of measurement: mm), which satisfies the absolute value | AIFS-AVFS | = | 0.02667mm | .

In the optical imaging system of this embodiment, the shortest working wavelength of visible light in the positive meridional fan diagram is incident on the first imaging plane through the edge of the aperture. The transverse aberration of 0.7 field of view is represented by PSTA, which is 0.00040mm, and is positive meridian. The longest working wavelength of visible light in the surface light fan chart is incident on the first imaging plane through the edge of the aperture. The transverse aberration of 0.7 field of view is expressed in PLTA, which is -0.009mm. The shortest working wavelength of visible light in the negative meridional light fan chart is through the aperture. The lateral aberration of 0.7 field of view incident on the first imaging plane at the edge is represented by NSTA, which is -0.002mm. The longest working wavelength of visible light in the negative meridional fan diagram is incident on the first imaging plane of 0.7 field of view through the edge of the aperture. The lateral aberration is represented by NLTA, which is -0.016 mm. The shortest working wavelength of the visible light of the sagittal plane fan chart is incident on the first imaging plane through the aperture edge. The transverse aberration of 0.7 field of view is represented by SSTA, which is 0.018mm. The longest working wavelength of the visible light of the sagittal plane fan chart is incident through the aperture edge. The lateral aberration of 0.7 field of view on the first imaging plane is represented by SLTA, which is 0.016 mm.

Refer to Tables 1 and 2 below for further cooperation.

According to Tables 1 and 2, the following values related to the length of the contour curve can be obtained:

Table 1 shows the detailed structural data of the first embodiment in FIG. 1, where the units of the radius of curvature, thickness, distance, and focal length are mm, and the surface 0-16 sequentially represents the surface from the object side to the image side. Table 2 shows the aspheric data in the first embodiment, where k represents the cone coefficient in the aspheric curve equation, and A1-A20 represents the aspherical coefficients of order 1-20 on each surface. In addition, the tables of the following embodiments are schematic diagrams and aberration curves corresponding to the embodiments. The definitions of the data in the tables are the same as the definitions of Tables 1 and 2 of the first embodiment, and will not be repeated here.

Second embodiment

Please refer to FIG. 2A and FIG. 2B. FIG. 2A illustrates a light according to a second embodiment of the present invention. The schematic diagram of the imaging system is shown in FIG. 2B. From left to right, the spherical aberration, astigmatism, and optical distortion curves of the optical imaging system of the second embodiment are sequentially shown. FIG. 2C is a transverse aberration diagram of the optical imaging system of the second embodiment at a 0.7 field of view. Figure 2D is a diagram showing the center-of-view, 0.3-field, and 0.7-field defocus modulation conversion contrast transfer rates of the visible light spectrum of this embodiment; Figure 2E is a diagram of the infrared light spectrum of the second embodiment of the present invention Defocus modulation conversion vs. transfer rate graph for the center field of view, 0.3 field of view, and 0.7 field of view. As can be seen from FIG. 2A, the optical imaging system includes the first lens 210, the second lens 220, the third lens 230, the aperture 200, the fourth lens 240, the fifth lens 250, and the sixth lens 260 in this order from the object side to the image side. And a seventh lens 270, an infrared filter 280, a first imaging surface 290, and an image sensing element 292.

The first lens 210 has a negative refractive power and is made of glass. The object side surface 212 is a convex surface, and the image side surface 214 is a concave surface. Both are aspherical surfaces.

The second lens 220 has a negative refractive power and is made of glass. The object side surface 222 is a convex surface, and the image side surface 224 is a concave surface, which are all aspheric surfaces.

The third lens 230 has a positive refractive power and is made of glass. Its object side surface 232 is a concave surface, and its image side surface 234 is a convex surface, which are all aspheric surfaces.

The fourth lens 240 has a positive refractive power and is made of glass. The object side surface 242 is a convex surface, and the image side surface 244 is a convex surface, and they are all aspheric surfaces.

The fifth lens 250 has a negative refractive power and is made of glass. Its object side surface 252 is concave, its image side surface 254 is concave, and all of them are aspheric, and its object side surface 252 has an inflection point.

The sixth lens 260 has a positive refractive power and is made of glass. Its object side 262 is convex, and its image side 264 is convex, and all of them are aspheric. Accordingly, the angle of incidence of each field of view on the sixth lens 260 can be effectively adjusted to improve aberrations.

The seventh lens 270 has a negative refractive power and is made of plastic. Its object side 272 is convex, its image side 274 is concave and both are aspheric, and its object side 272 has a curved point and the image side 274 has two Inflection point. Thereby, it is advantageous to shorten the back focal length to maintain miniaturization. In addition, it can effectively suppress the incident angle of the off-axis field of view, and further correct the aberration of the off-axis field of view.

The infrared filter 280 is made of glass and is disposed between the seventh lens 270 and the first imaging surface 290 without affecting the focal length of the optical imaging system.

Please refer to Tables 3 and 4 below.

In the second embodiment, the aspherical curve equation is expressed as the first embodiment. In addition, the definitions of the parameters in the following table are the same as those in the first embodiment, and will not be repeated here.

According to Table 3 and Table 4, the following conditional formula values can be obtained:

According to Tables 3 and 4, the following values related to the length of the contour curve can be obtained:

According to Table 3 and Table 4, the following conditional formula values can be obtained:

Third embodiment

Please refer to FIG. 3A and FIG. 3B, wherein FIG. 3A shows a schematic diagram of an optical imaging system according to a third embodiment of the present invention, and FIG. 3B shows the optical imaging system of the third embodiment in order from left to right. Spherical aberration, astigmatism and optical distortion curves. Fig. 3C shows the optical imaging system of the third embodiment at 0.7 Horizontal aberration diagram at the field. Fig. 3D is a diagram showing the central field of view, 0.3 field of view, and 0.7 field of view of the visible spectrum of the present embodiment with defocus modulation conversion and transfer rate; Fig. 3E is a diagram illustrating the infrared spectrum of the second embodiment of the present invention Defocus modulation conversion vs. transfer rate graph for the center field of view, 0.3 field of view, and 0.7 field of view. As can be seen from FIG. 3A, the optical imaging system includes a first lens 310, a second lens 320, a third lens 330, an aperture 300, a fourth lens 340, a fifth lens 350, and a sixth lens 360 in order from the object side to the image side. And a seventh lens 370, an infrared filter 380, a first imaging surface 390, and an image sensing element 392.

The first lens 310 has a negative refractive power and is made of glass. The object side surface 312 is a convex surface, and the image side surface 314 is a concave surface, and they are all aspheric surfaces.

The second lens 320 has a negative refractive power and is made of glass. Its object side 322 is convex, its image side 324 is concave, and both are aspheric. Its object side 322 has a point of inflection.

The third lens 330 has a positive refractive power and is made of glass. The object side surface 332 is a concave surface, and the image side surface 334 is a convex surface.

The fourth lens 340 has a positive refractive power and is made of glass. The object side surface 342 is a convex surface, and the image side surface 344 is a convex surface, which are all aspheric surfaces.

The fifth lens 350 has a negative refractive power and is made of plastic. The object side 352 is convex, the image side 354 is concave, and both are aspheric. The object side 352 and the image side 354 both have an inflection point.

The sixth lens 360 has a positive refractive power and is made of plastic. The object side 362 is convex, and the image side 364 is convex, and all of them are aspheric. This can effectively adjust the angle of incidence of each field of view on the sixth lens 360 to improve aberrations.

The seventh lens 370 has a negative refractive power and is made of plastic. Its object side surface 372 is concave, and its image side surface 374 is concave, and all of them are aspheric. Thereby, it is advantageous to shorten the back focal length to maintain miniaturization. In addition, it can effectively suppress the incident angle of the off-axis field of view, and further correct the aberration of the off-axis field of view.

The infrared filter 380 is made of glass and is disposed between the seventh lens 370 and the first imaging surface 390 without affecting the focal length of the optical imaging system.

Please refer to Table 5 and Table 6 below.

In the third embodiment, the aspherical curve equation is expressed as the first embodiment. In addition, the definitions of the parameters in the following table are the same as those in the first embodiment, and will not be repeated here.

According to Table 5 and Table 6, the following conditional formula values can be obtained:

According to Table 5 and Table 6, the following values related to the length of the contour curve can be obtained:

According to Table 5 and Table 6, the following conditional formula values can be obtained:

Fourth embodiment

Please refer to FIG. 4A and FIG. 4B. FIG. 4A shows a schematic diagram of an optical imaging system according to a fourth embodiment of the present invention. FIG. Spherical aberration, astigmatism and optical distortion curves. FIG. 4C is a lateral aberration diagram of the optical imaging system of the fourth embodiment at a 0.7 field of view. FIG. 4D is a diagram showing the defocus modulation conversion contrast transfer rate of the central field of view, 0.3 field of view, and 0.7 field of view of the visible light spectrum of the present embodiment; FIG. 4E is a second embodiment of the present invention The center field of view, 0.3 field of view, 0.7 field of view of the infrared light spectrum of the defocus modulation conversion contrast transfer rate chart. As can be seen from FIG. 4A, the optical imaging system includes a first lens 410, a second lens 420, a third lens 430, an aperture 400, a fourth lens 440, a fifth lens 450, and a sixth lens 460 in order from the object side to the image side. And a seventh lens 470, an infrared filter 480, a first imaging surface 490, and an image sensing element 492.

The first lens 410 has a negative refractive power and is made of glass. The object side surface 412 is a convex surface, and the image side surface 414 is a concave surface. Both are aspherical surfaces.

The second lens 420 has a negative refractive power and is made of glass. The object side surface 422 is a convex surface, and the image side surface 424 is a concave surface, which are all aspheric surfaces.

The third lens 430 has a positive refractive power and is made of glass. The object side surface 432 is a concave surface, and the image side surface 434 is a convex surface, which are all aspheric surfaces.

The fourth lens 440 has a positive refractive power and is made of glass. The object side 442 is convex, and the image side 444 is convex, and all of them are aspheric.

The fifth lens 450 has a negative refractive power and is made of plastic. Its object side surface 452 is concave, its image side 454 is concave, and both are aspheric. Its image side 452 has two inflection points.

The sixth lens 460 has a positive refractive power and is made of a plastic material. Its object side 462 is convex, and its image side 464 is convex, and all of them are aspheric. Thereby, the angle of incidence of each field of view on the sixth lens 460 can be effectively adjusted to improve aberrations.

The seventh lens 470 has a negative refractive power and is made of a plastic material. Its object side surface 472 is a concave surface, and its image side surface 474 is a convex surface, which are all aspheric surfaces. Thereby, it is advantageous to shorten the back focal length to maintain miniaturization. In addition, both the object side surface 472 and the image side surface 474 have an inflection point, which can effectively suppress the incident angle of the off-axis field of view, and further correct the aberration of the off-axis field of view.

The infrared filter 480 is made of glass and is disposed between the seventh lens 470 and the first imaging surface 490 without affecting the focal length of the optical imaging system.

Please refer to Table 7 and Table 8 below.

In the fourth embodiment, the curve equation of the aspherical surface is expressed as the first embodiment. In addition, the definitions of the parameters in the following table are the same as those in the first embodiment, and will not be repeated here.

According to Table 7 and Table 8, the following conditional formula values can be obtained:

According to Tables 7 and 8, the following values related to the length of the contour curve can be obtained:

According to Table 7 and Table 8, the following conditional formula values can be obtained:

Fifth Embodiment

Please refer to FIG. 5A and FIG. 5B, wherein FIG. 5A shows a schematic diagram of an optical imaging system according to a fifth embodiment of the present invention, and FIG. 5B shows the optical imaging system of the fifth embodiment in order from left to right. Spherical aberration, astigmatism and optical distortion curves. FIG. 5C is a transverse aberration diagram of the optical imaging system of the fifth embodiment at a 0.7 field of view. Fig. 5D is a diagram showing the central field of view, 0.3 field of view, and 0.7 field of view of the visible spectrum of the present embodiment with defocus modulation conversion and transfer rate; Fig. 5E is a diagram illustrating the infrared spectrum of the second embodiment of the present invention Defocus modulation conversion vs. transfer rate graph for the center field of view, 0.3 field of view, and 0.7 field of view. It can be seen from FIG. 5A that the optical imaging system includes the first lens 510 and the second lens in order from the object side to the image side. 520, third lens 530, aperture 500, fourth lens 540, fifth lens 550, sixth lens 560, and seventh lens 570, infrared filter 580, first imaging surface 590, and image sensing element 592.

The first lens 510 has a negative refractive power and is made of glass. Its object side 512 is convex, its image side 514 is concave, and both are aspheric.

The second lens 520 has a negative refractive power and is made of glass. The object side 522 is concave, the image side 524 is concave, and both are aspheric. The object side 522 has a point of inflection.

The third lens 530 has a positive refractive power and is made of glass. Its object side 532 is convex, its image side 534 is convex, and both are aspheric. Its object side 532 has a point of inflection.

The fourth lens 540 has a positive refractive power and is made of plastic. Its object side surface 542 is convex, its image side surface 544 is convex, and both are aspheric. Its object side surface 542 has a inflection point.

The fifth lens 550 has a negative refractive power and is made of plastic. The object side 552 is concave, the image side 554 is concave, and both are aspheric. The object side 552 has an inflection point and the image side 554 has two points. Inflection point.

The sixth lens 560 has a positive refractive power and is made of plastic. The object side surface 562 is convex, the image side 564 is convex, and both are aspheric. The object side 562 has an inflection point. Thereby, the angle of incidence of each field of view on the sixth lens 560 can be effectively adjusted to improve aberrations.

The seventh lens 570 has a negative refractive power and is made of plastic. Its object side surface 572 is concave, its image side 574 is convex, and its object side 572 and image side 574 both have a point of inflection. Thereby, it is advantageous to shorten the back focal length to maintain miniaturization. In addition, it can effectively suppress the incident angle of the off-axis field of view and correct the aberrations of the off-axis field of view.

The infrared filter 580 is made of glass and is disposed between the seventh lens 570 and the first imaging surface 590 without affecting the focal length of the optical imaging system.

Please refer to Tables 9 and 10 below.

In the fifth embodiment, the aspherical curve equation is expressed as the first embodiment. In addition, the definitions of the parameters in the following table are the same as those in the first embodiment, and will not be repeated here.

According to Table 9 and Table 10, the following conditional formula values can be obtained:

According to Tables 9 and 10, the following values related to the length of the contour curve can be obtained:

According to Table 9 and Table 10, the following conditional formula values can be obtained:

Sixth embodiment

Please refer to FIG. 6A and FIG. 6B, wherein FIG. 6A shows a schematic diagram of an optical imaging system according to a sixth embodiment of the present invention, and FIG. 6B shows the optical imaging system of the sixth embodiment in order from left to right. Spherical aberration, astigmatism and optical distortion curves. FIG. 6C is a transverse aberration diagram of the optical imaging system of the sixth embodiment at a 0.7 field of view. FIG. 6D is a diagram showing the center-of-view, 0.3-field, and 0.7-field defocus modulation conversion contrast transfer ratio of the visible light spectrum of this embodiment; FIG. 6E is a diagram of the infrared light spectrum of the second embodiment of the present invention Defocus modulation conversion vs. transfer rate graph for the center field of view, 0.3 field of view, and 0.7 field of view. It can be seen from FIG. 6A that the optical imaging system includes a first lens 610, a second lens 620, a third lens 630, an aperture 600, a fourth lens 640, a fifth lens 650, and a sixth lens 660 in order from the object side to the image side. , A seventh lens 670, an infrared filter 680, a first imaging surface 690, and an image sensing element 692.

The first lens 610 has a negative refractive power and is made of glass. Its object-side surface 612 is convex, its image-side 614 is concave, and both are aspherical.

The second lens 620 has a negative refractive power and is made of glass. Its object side 622 is convex, its image side 624 is concave, and both are aspheric. Its object side 622 has a point of inflection.

The third lens 630 has a positive refractive power and is made of a plastic material. Its object side 632 is concave, its image side 634 is convex, and all of them are aspheric.

The fourth lens 640 has a positive refractive power and is made of a plastic material. Its object side 642 is convex, and its image side 644 is convex, and all of them are aspheric.

The fifth lens 650 has a negative refractive power and is made of plastic. The object side surface 652 is a concave surface, and the image side surface 654 is a concave surface.

The sixth lens 660 has a positive refractive power and is made of a plastic material. Its object side 662 is convex, and its image side 664 is convex, and they are all aspheric. This can effectively adjust the angle of incidence of each field of view on the sixth lens 660 to improve aberrations.

The seventh lens 670 has a negative refractive power and is made of plastic material. Its object side surface 672 is concave, its image side 674 is concave, and its image side 674 has an inflection point. Thereby, it is advantageous to shorten the back focal length to maintain miniaturization. In addition, it can also effectively suppress the angle of incidence of the off-axis field of view, and further correct the aberration of the off-axis field of view.

The infrared filter 680 is made of glass and is disposed between the seventh lens 670 and the first imaging surface 690 without affecting the focal length of the optical imaging system.

Please refer to Table 11 and Table 12 below.

In the sixth embodiment, the curve equation of the aspherical surface is expressed as the first embodiment. In addition, the definitions of the parameters in the following table are the same as those in the first embodiment, and will not be repeated here.

According to Table 11 and Table 12, the following conditional formula values can be obtained:

According to Table 11 and Table 12, the following values related to the length of the contour curve can be obtained:

According to Table 11 and Table 12, the following conditional formula values can be obtained:

Although the present invention has been disclosed in the above embodiments, it is not intended to limit the present invention. Any person skilled in the art can make various modifications and retouches without departing from the spirit and scope of the present invention. Therefore, the protection of the present invention The scope shall be determined by the scope of the attached patent application.

Although the present invention has been particularly shown and described with reference to exemplary embodiments thereof, it will be understood by those having ordinary knowledge in the art that the spirit of the present invention as defined by the scope of the following patent applications and their equivalents will be understood Various changes in form and detail can be made under the categories.

Claims (25)

An optical imaging system includes: a first lens having a refractive power; a second lens having a refractive power; a third lens having a refractive power; a fourth lens having a refractive power A fifth lens with a refractive power; a sixth lens with a refractive power; a seventh lens with a refractive power; a first imaging plane; a visible light image plane perpendicular to the optical axis and its center The defocus modulation conversion contrast ratio (MTF) of the field of view at the first spatial frequency has a maximum value; and a second imaging plane; it is a specific infrared light image plane perpendicular to the optical axis and its central field of view is There is a maximum value of the defocus modulation conversion contrast transfer rate (MTF) of a spatial frequency, wherein the optical imaging system has seven lenses having refractive power, and at least one of the first lens to the seventh lens is made of plastic and The material of at least one lens is glass, and at least one of the first lens to the seventh lens has a positive refractive power, and the focal lengths of the first lens to the seventh lens are f1, f2, f3, f4, f5, and f6, respectively. , F7, the The focal length of the imaging system is f, the entrance pupil diameter of the optical imaging system is HEP, the distance from the object side of the first lens to the first imaging plane on the optical axis is HOS, and the distance from the object side of the first lens to the seventh The lens image side has a distance InTL on the optical axis, half of the maximum viewing angle of the optical imaging system is HAF, the optical imaging system has a maximum imaging height HOI perpendicular to the optical axis on the first imaging plane, and the first The distance between the imaging surface and the second imaging surface on the optical axis is FS, which satisfies the following conditions: 1.0 ≦ f / HEP ≦ 10.0; 0deg <HAF ≦ 150deg, and | FS | ≦ 60 μm. The optical imaging system according to claim 1, wherein the infrared light has a wavelength between 700 nm and 1300 nm and the first spatial frequency is expressed by SP1, which satisfies the following conditions: SP1 ≦ 440 cycles / mm. The optical imaging system according to claim 1, wherein the intersection point between any surface of any of the lenses and the optical axis is a starting point, and the contour of the surface is extended until the surface is 1/2 of the entrance pupil diameter from the optical axis Up to the coordinate point at the vertical height, the length of the contour curve between the aforementioned two points is ARE, which satisfies the following conditions: 1 ≦ 2 (ARE / HEP) ≦ 2.0. The optical imaging system according to claim 1, wherein a material of at least two lenses of the first lens to the seventh lens is plastic. The optical imaging system according to claim 1, wherein the third lens has a positive refractive power, and an image side of the third lens is convex on the optical axis. The optical imaging system according to claim 1, wherein at least one surface of each of at least one of the first lens to the seventh lens has at least one inflection point. The optical imaging system according to claim 1, wherein the intersection of the object side of the seventh lens on the optical axis is the starting point, and extends along the contour of the surface until the vertical height of the surface is 1/2 of the entrance pupil diameter from the optical axis. The coordinate curve length between the above two points is ARE71, the intersection of the image side of the seventh lens on the optical axis is the starting point, and the contour of the surface is extended until the surface is 1/2 incident from the optical axis. Up to the coordinate point at the vertical height of the pupil diameter, the length of the contour curve between the two points is ARE72, and the thickness of the seventh lens on the optical axis is TP7, which satisfies the following conditions: 0.05 ≦ ARE71 / TP7 ≦ 35; and 0.05 ≦ ARE72 / TP7 ≦ 35. The optical imaging system according to claim 1, wherein the TV of the optical imaging system is deformed to TDT at the time of image formation, and the longest working wavelength of the positive meridional fan of the optical imaging system passes through the edge of the entrance pupil and is incident on the The lateral aberration at 0.7HOI on the first imaging plane is represented by PLTA. The shortest working wavelength of the positive meridional fan passes through the edge of the entrance pupil and is incident on the first imaging plane at 0.7HOI. The lateral aberration is represented by PSTA. Indicates that the longest working wavelength of the negative meridional fan passes through the edge of the entrance pupil and is incident on the first imaging plane at 0.7HOI. The lateral aberration is represented by NLTA, and the shortest working wavelength of the negative meridional fan passes through the incident. The lateral aberration of the pupil edge and incident on the first imaging plane at 0.7HOI is represented by NSTA. The longest working wavelength of the sagittal plane fan passes through the incident pupil edge and incident on the first imaging plane at 0.7HOI. The difference is represented by SLTA. The shortest working wavelength of the sagittal plane fan passes through the edge of the entrance pupil and is incident on the first imaging plane at 0.7HOI. The lateral aberration is represented by SSTA, which satisfies the following conditions: PLTA ≦ 100 microns; PSTA 100 microns; NLTA ≦ 100 micrometers; NSTA ≦ 100 micrometers; SLTA ≦ 100 micrometers; and SSTA ≦ 100 micrometers; | TDT | <100%. The optical imaging system according to claim 1, further comprising an aperture, and a distance InS on the optical axis from the aperture to the first imaging plane, which satisfies the following formula: 0.2 ≦ InS / HOS ≦ 1.1. An optical imaging system includes: a first lens having a refractive power; a second lens having a refractive power; a third lens having a refractive power; a fourth lens having a refractive power A fifth lens with a refractive power; a sixth lens with a refractive power; a seventh lens with a refractive power; a first imaging plane; a visible light image plane perpendicular to the optical axis and its center The field of view has a maximum defocus modulation conversion contrast transfer ratio (MTF) at the first spatial frequency (110 cycles / mm); and a second imaging plane; it is a specific infrared light image plane perpendicular to the optical axis and its The central field of view has a maximum defocus modulation conversion contrast transfer rate (MTF) at the first spatial frequency (110 cycles / mm), where the optical imaging system has seven lenses with refractive power, from the first lens to the seventh The material of at least one lens in the lens is plastic and the material of at least one lens is glass. The optical imaging system has a maximum imaging height HOI perpendicular to the optical axis on the first imaging plane. The first lens to the seventh lens to A lens has a positive refractive power, and the focal lengths of the first lens to the seventh lens are f1, f2, f3, f4, f5, f6, and f7, the focal length of the optical imaging system is f, and the entrance pupil of the optical imaging system The diameter is HEP. The distance from the object side of the first lens to the first imaging plane is HOS on the optical axis. The distance from the object side of the first lens to the image side of the seventh lens has a distance InTL on the optical axis. The optical imaging Half of the maximum viewing angle of the system is HAF, the distance between the first imaging surface and the second imaging surface on the optical axis is FS, and the intersection of any surface of any of the lenses with the optical axis is the starting point. Extend the contour of the surface until the coordinate point on the surface at the vertical height of 1/2 of the entrance pupil diameter from the optical axis. The length of the contour curve between the two points is ARE, which meets the following conditions: 1.0 ≦ f / HEP ≦ 10.0; 0deg <HAF ≦ 150deg; | FS | ≦ 60μm and 1 ≦ 2 (ARE / HEP) ≦ 2.0. The optical imaging system according to claim 10, wherein the maximum effective radius of any surface of any one of the lenses is represented by EHD, and the intersection of any surface of any one of the lenses with the optical axis is a starting point, Extend the contour of the surface until the maximum effective radius of the surface is the end point. The length of the contour curve between the two points is ARS, which satisfies the following formula: 1 ≦ ARS / EHD ≦ 2.0. The optical imaging system according to claim 10, wherein each of the lenses has an air gap. The optical imaging system according to claim 10, wherein a distance on the optical axis between the third lens and the fourth lens is IN34, and a distance between the fourth lens and the fifth lens on the optical axis is IN45, the distance on the optical axis between the fifth lens and the sixth lens is IN56, which satisfies the following formulas: IN34 ≧ IN45 and IN34 ≧ IN56. The optical imaging system according to claim 10, wherein a material of at least two lenses of the first lens to the seventh lens is plastic. The optical imaging system according to claim 10, wherein the first lens has a negative refractive power, and an image side thereof is concave on an optical axis. The optical imaging system according to claim 10, wherein the third lens has a positive refractive power, and its image side is convex on the optical axis. The optical imaging system according to claim 10, wherein the image side of the second lens is concave on the optical axis. The optical imaging system according to claim 10, wherein at least one of the first lens, the second lens, the third lens, the fourth lens, the fifth lens, the sixth lens, and the seventh lens has a wavelength smaller than 500nm light filter element. The optical imaging system according to claim 10, wherein the distance between the sixth lens and the seventh lens on the optical axis is IN67, and the thicknesses of the sixth lens and the seventh lens on the optical axis are TP6 and TP7, which satisfies the following conditions: 0.1 ≦ (TP7 + IN67) / TP6 ≦ 50. An optical imaging system includes: a first lens having a refractive power; a second lens having a refractive power; a third lens having a refractive power; a fourth lens having a refractive power A fifth lens having a refractive power; a sixth lens having a refractive power; a seventh lens having a refractive power; a first average imaging plane; a visible light image plane perpendicular to the optical axis and set The average position of the out-of-focus position of each of the central field of view, 0.3 field of view, and 0.7 field of view of the optical imaging system at the first spatial frequency (110 cycles / mm) with the maximum MTF value of the field of view; and a second average Imaging plane; it is a specific infrared light image plane perpendicular to the optical axis and is set in the central field of view, 0.3 field of view, and 0.7 field of view of the optical imaging system, each of which has a first space frequency (110 cycles / mm). The average position of the defocus position of the maximum MTF value of the field of view, wherein the optical imaging system has seven lenses having refractive power, and at least one of the first lens to the seventh lens is made of plastic and at least one lens. The material is glass, the optical imaging system has a maximum imaging height HOI perpendicular to the optical axis on the first average imaging surface, and the focal lengths of the first lens to the seventh lens are f1, f2, f3, f4, f5, f6, f7, the focal length of the optical imaging system is f, the entrance pupil diameter of the optical imaging system is HEP, half of the maximum viewing angle of the optical imaging system is HAF, the first lens object side to the first average imaging surface is There is a distance HOS on the optical axis, the distance from the object side of the first lens to the image side of the sixth lens has a distance InTL on the optical axis, and the distance between the first average imaging plane and the second average imaging plane is AFS. The intersection of any surface of any of these lenses with the optical axis is the starting point, and extends the contour of the surface until the coordinate point on the surface at a vertical height of 1/2 of the entrance pupil diameter of the optical axis. The contour curve length is ARE, which satisfies the following conditions: 1 ≦ f / HEP ≦ 10; 0deg <HAF ≦ 150deg; | AFS | ≦ 60μm and 1 ≦ 2 (ARE / HEP) ≦ 2.0. The optical imaging system according to claim 10, wherein the maximum effective radius of any surface of any one of the lenses is represented by EHD, and the intersection of any surface of any one of the lenses with the optical axis is a starting point, Extend the contour of the surface until the maximum effective radius of the surface is the end point. The length of the contour curve between the two points is ARS, which satisfies the following formula: 1 ≦ ARS / EHD ≦ 2.0. The optical imaging system according to claim 20, wherein each of the lenses has an air gap. The optical imaging system according to claim 20, wherein a distance on the optical axis between the third lens and the fourth lens is IN34, and a distance on the optical axis between the fourth lens and the fifth lens is IN45, the distance on the optical axis between the fifth lens and the sixth lens is IN56, which satisfies the following formulas: IN34 ≧ IN45 and IN34 ≧ IN56. The optical imaging system according to claim 20, wherein the image side of the third lens is convex on the optical axis. The optical imaging system according to claim 20, wherein the optical imaging system further includes an aperture and an image sensing element, the image sensing element is disposed behind the first average imaging surface and is provided with at least 100,000 pixels, and There is a distance InS on the optical axis from the aperture to the first average imaging plane, which satisfies the following formula: 0.2 ≦ InS / HOS ≦ 1.1.