TWM600850U - Optical image capturing system - Google Patents

Abstract

The invention discloses a four-piece optical lens for capturing image and a five-piece optical module for capturing image. In order from an object side to an image side, the optical lens along the optical axis comprises a first lens with positive refractive power; a second lens with refractive power; a third lens with refractive power; and a fourth lens with refractive power; and at least one of the image-side surface and object-side surface of each of the four lens elements are aspheric. The optical lens can increase aperture value and improve the imagining quality for use in compact cameras.

Description

Optical imaging system

This creation is about an optical imaging system, and especially about a miniaturized optical imaging system applied to electronic products.

In recent years, with the rise of portable electronic products with photography functions, the demand for optical systems has increased day by day. The photosensitive elements of general optical systems are nothing more than Charge Coupled Device (CCD) or Complementary Metal-Oxide Semiconductor Sensor (CMOS Sensor). With the advancement of semiconductor manufacturing technology, The pixel size of the photosensitive element has been reduced, and the optical system has gradually developed into the field of high pixels, so the requirements for image quality are also increasing.

Traditional optical systems mounted on portable devices mostly use two or three-element lens structures. However, as portable devices continue to improve their pixels and end consumers’ needs for large apertures such as low light and night Shooting function or the need for wide viewing angle, such as the Selfie function of the front lens. However, the design of a large aperture optical system often faces the situation of generating more aberrations, which will degrade the surrounding imaging quality and the difficulty of manufacturing, while the design of a wide viewing angle optical system will face an increase in the imaging distortion rate (distortion). The optical imaging system has been unable to meet the higher-level photography requirements.

Therefore, how to effectively increase the light input of the optical imaging system and increase the viewing angle of the optical imaging system, in addition to further improving the total pixels and quality of imaging, while also taking into account the balance design of the miniaturized optical imaging system, has become a very important issue.

The aspect of this creative embodiment is aimed at an optical imaging system that can utilize the refractive power of four lenses, the combination of convex and concave surfaces (the convex or concave surface in this creation refers in principle to the object side or image side of each lens on the optical axis Described on the geometric shape), and effectively improve the optical performance The amount of light entering the imaging system and the viewing angle of the optical imaging system are increased, while the total pixels and quality of the imaging are improved for use in small electronic products.

The terms and codes of the lens parameters related to this creative embodiment are listed below for reference in the subsequent description: lens parameters related to length or height. The imaging height of the optical imaging system is represented by HOI; the height of the optical imaging system is represented by HOS; optics The distance between the object side of the first lens and the image side of the fourth lens of the imaging system is expressed in InTL; the distance between the image side of the fourth lens of the optical imaging system and the imaging surface is expressed in InB; InTL+InB=HOS; of the optical imaging system The distance between the fixed diaphragm (aperture) and the 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 Represented by TP1 (example).

Material-related lens parameters The dispersion coefficient of the first lens of the optical imaging system is represented by NA1 (example); the refractive index of the first lens is represented by Nd1 (example).

Lens parameters related to the viewing angle are expressed in AF; half of the viewing angle is expressed in HAF; and the chief ray angle is expressed in MRA.

Lens parameters related to the entrance and exit pupil. The entrance pupil diameter of an optical imaging system is expressed in HEP; the maximum effective radius of any surface of a single lens refers to the intersection point of the system's maximum angle of view, the incident light passing through the edge of the entrance pupil and the lens surface (EffectiveHalfDiameter ; EHD), the vertical height between the intersection point 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 expression of the maximum effective radius of any surface of the remaining lenses in the optical imaging system can be deduced by analogy.

Parameters related to the depth of the lens surface. The horizontal displacement distance from the intersection of the object side surface of the fourth lens on the optical axis to the position of the maximum effective radius of the object side surface of the fourth lens on the optical axis is represented by InRS41 (example); The horizontal displacement distance from the intersection on the optical axis to the maximum effective radius position of the image side surface of the fourth lens and the optical axis is represented by InRS42 (example).

Parameters related to lens surface Critical point C refers to a point on the surface of a specific lens that is tangent to a tangent plane perpendicular to the optical axis, except for the point of intersection with the optical axis. Continuing, for example, the vertical distance between the critical point C31 on the object side of the third lens and the optical axis is HVT31 (example), the vertical distance between the critical point C32 on the image side of the third lens and the optical axis is HVT32 (example), and the fourth lens object The vertical distance between the critical point C41 on the side surface and the optical axis is HVT41 (example), and the vertical distance between the critical point C42 on the side surface of the fourth lens and the optical axis is HVT42 (example). For other lenses, the critical points on the object side or the image side and the vertical distance from the optical axis are expressed in the same way as described above.

The inflection point closest to the optical axis on the object side of the fourth lens is IF411. The sinking amount of this point is SGI411 (example). SGI411 is the intersection of the object side of the fourth lens on the optical axis to the nearest optical axis of the object side of the fourth lens. The horizontal displacement distance between the inflection points parallel to the optical axis, the vertical distance between this point and the optical axis of IF411 is HIF411 (example). The inflection point closest to the optical axis on the image side of the fourth lens is IF421. The sinking amount of this point is SGI421 (example). SGI411 is the intersection of the image side of the fourth lens on the optical axis to the closest optical axis of the image side of the fourth lens. The horizontal displacement distance between the inflection points parallel to the optical axis, the vertical distance between this point and the optical axis of IF421 is HIF421 (example).

The second inflection point on the object side of the fourth lens that is close to the optical axis is IF412. The sinking amount of this point is SGI412 (example). SGI412 is the intersection of the object side of the fourth lens on the optical axis and the second closest to the object side of the fourth lens. The horizontal displacement distance between the inflection points of the optical axis parallel to the optical axis, and the vertical distance between this point of IF412 and the optical axis is HIF412 (example). The second inflection point on the image side of the fourth lens that is closest to the optical axis is IF422. The sinking amount of this point is SGI422 (example). SGI422 is the intersection of the image side of the fourth lens on the optical axis and the second closest to the image side of the fourth lens. The horizontal displacement distance between the inflection point of the optical axis parallel to the optical axis, and the vertical distance between this point of IF422 and the optical axis is HIF422 (example).

The third inflection point on the object side of the fourth lens that is close to the optical axis is IF413. The sinking amount of this point is SGI413 (example). SGI413 is the intersection point of the object side of the fourth lens on the optical axis to the third closest to the object side of the fourth lens. The horizontal displacement distance between the inflection points of the optical axis parallel to the optical axis, and the vertical distance between this point of IF4132 and the optical axis is HIF413 (example). The third inflection point on the image side of the fourth lens that is close to the optical axis is IF423. The sinking amount of this point is SGI423 (example). SGI423 is the intersection of the image side of the fourth lens on the optical axis and the third closest to the image side of the fourth lens. The horizontal displacement distance between the inflection points of the optical axis parallel to the optical axis, and the vertical distance between this point of IF423 and the optical axis is HIF423 (example).

The fourth inflection point close to the optical axis on the object side of the fourth lens is IF414. The sinking amount of this point is SGI414 (example). SGI414 is the intersection of the object side of the fourth lens on the optical axis to the fourth lens. The horizontal displacement distance between the fourth inflection point close to the optical axis on the side of the lens and the optical axis is parallel, and the vertical distance between this point of IF414 and the optical axis is HIF414 (example). The fourth inflection point on the image side of the fourth lens that is close to the optical axis is IF424. The sinking amount of this point is SGI424 (example). SGI424 is the intersection point of the image side of the fourth lens on the optical axis to the fourth closest to the image side of the fourth lens. The horizontal displacement distance between the inflection points of the optical axis parallel to the optical axis, and the vertical distance between this point of IF424 and the optical axis is HIF424 (example).

The expression of the inflection point on the object side or the image side of the other lens and the vertical distance from the optical axis or the sinking amount of the lens is similar to the foregoing.

The aberration-related variables Optical Distortion (Optical Distortion) of the optical imaging system is expressed in ODT; its TV Distortion (TV Distortion) is expressed in TDT, and can be further defined to describe the aberration shift between 50% and 100% of the imaging field Degree; the spherical aberration offset is expressed in DFS; the coma aberration offset is expressed in DFC.

The Modulation Transfer Function (MTF) of the optical imaging system is used to test and evaluate the contrast and sharpness of the system imaging. The vertical axis of the modulation transfer function characteristic diagram represents the contrast transfer rate (value from 0 to 1), and the horizontal axis represents the spatial frequency (cycles/mm; lp/mm; line pairs per mm). The perfect imaging system can theoretically show 100% line contrast of the subject, but the actual imaging system has a contrast transfer rate value of less than 1 on the vertical axis. In addition, generally speaking, the edge area of the image is more difficult to obtain fine reduction than the center area. The visible light spectrum is on the imaging surface. The contrast transfer rate (MTF value) of the optical axis, 0.3 field of view, and 0.7 field of view at a spatial frequency of 55 cycles/mm is represented by MTFE0, MTFE3, and MTFE7, respectively. Optical axis, 0.3 field of view, and 0.7 field of view The contrast transfer rate (MTF value) of field 3 at the spatial frequency of 110 cycles/mm is represented by MTFQ0, MTFQ3 and MTFQ7 respectively, and the contrast transfer rate (MTF value) of the optical axis, 0.3 field of view and 0.7 field of view at the spatial frequency of 220 cycles/mm Expressed as MTFH0, MTFH3, and MTFH7, the contrast transfer rate (MTF value) of the optical axis, 0.3 field of view, and 0.7 field of view at a spatial frequency of 440 cycles/mm are expressed as MTF0, MTF3, and MTF7, respectively. The center, inner field of view, and outer field of view of the lens are representative, so it can be used to evaluate the performance of a specific optical imaging system. If the design of the optical imaging system corresponds to the pixel size (Pixel Size) containing the photosensitive element less than 1.12 microns, so the modulation transfer function characteristic diagram of the quarter spatial frequency, half the spatial frequency (half frequency) and the full spatial frequency ( Full frequency) at least 110cycles/mm, 220cycles/mm and 440cycles/mm.

If the optical imaging system must also meet the imaging requirements of the infrared spectrum, such as night vision requirements for low light sources, the working wavelength used can be 850nm or 800nm. Because the main function is to identify the contours of objects formed by black and white light and dark, high resolution is not required Therefore, it is only necessary to select a spatial frequency less than 110 cycles/mm to evaluate the performance of a specific optical imaging system in the infrared spectrum. When the aforementioned working wavelength of 850nm is focused on the imaging surface, the contrast transfer rate (MTF value) of the image at the optical axis, 0.3 field of view, and 0.7 field of view at a spatial frequency of 55 cycles/mm is represented by MTFI0, MTFI3, and MTFI7, respectively. However, because the infrared operating wavelength of 850nm or 800nm is far from the general visible light wavelength, if the optical imaging system needs to focus on visible light and infrared (dual mode) at the same time and achieve certain performance, it is quite difficult to design.

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

According to the present creation, an optical imaging system is provided, which includes a first lens, a second lens, a third lens, a fourth lens, and an imaging surface in sequence from the object side to the image side. The first lens has refractive power. The focal lengths of the first lens to the fourth lens are f1, f2, f3, f4, the focal length of the optical imaging system is f, the entrance pupil diameter of the optical imaging system is HEP, and the object side of the first lens is to the imaging The surface has a distance HOS on the optical axis, the object side of the first lens to the image side of the fourth lens has a distance of InTL on the optical axis, half of the maximum viewing angle of the optical imaging system is HAF, and the first lens to The thickness of the fourth lens at the height of 1/2HEP and parallel to the optical axis are ETP1, ETP2, ETP3, ETP4, the sum of the aforementioned ETP1 to ETP4 is SETP, and the thickness of the first lens to the fourth lens on the optical axis are respectively TP1, TP2, TP3, TP4, the sum of the aforementioned TP1 to TP4 is STP, which meets the following conditions: 1.0≦f/HEP≦10.0; 0deg<HAF≦150deg and 0.5≦SETP/STP<1.

According to the present creation, another optical imaging system is provided, which includes a first lens, a second lens, a third lens, a fourth lens, and an imaging surface in sequence from the object side to the image side. The first lens has refractive power. The second lens has refractive power. The third lens has refractive power. The fourth lens has refractive power. At least two of the first lens to the fourth lens have at least one surface respectively At least one inflection point, and at least one of the second lens to the fourth lens has a positive refractive power, the focal lengths of the first lens to the fourth lens are f1, f2, f3, and f4, respectively, the optical imaging system The focal length of the optical imaging system is f, the entrance pupil diameter of the optical imaging system is HEP, the object side of the first lens to the imaging surface has a distance HOS on the optical axis, and the object side of the first lens to the image side of the fourth lens is There is a distance InTL on the axis, half of the maximum viewing angle of the optical imaging system is HAF, and the horizontal distance between the coordinate point on the object side of the first lens at 1/2HEP height and the imaging plane parallel to the optical axis is ETL, The horizontal distance between the coordinate point at 1/2HEP height on the object side of the first lens and the coordinate point at 1/2HEP height on the image side of the fourth lens parallel to the optical axis is EIN, which satisfies the following conditions: 1.0≦f /HEP≦10.0; 0deg<HAF≦150deg and 0.2≦EIN/ETL<1.

According to the present creation, an optical imaging system is provided, which includes a first lens, a second lens, a third lens, a fourth lens, and an imaging surface in sequence from the object side to the image side. At least one of the object side surface and the image side surface of the fourth lens has at least one inflection point, and the optical imaging system has four lenses with refractive power. The first lens has negative refractive power. The second lens has refractive power. The third lens has refractive power. The fourth lens has refractive power. The focal lengths of the first lens to the fourth lens are f1, f2, f3, f4, the focal length of the optical imaging system is f, the entrance pupil diameter of the optical imaging system is HEP, and the object side of the first lens is to the imaging The surface has a distance HOS on the optical axis, the object side of the first lens to the image side of the fourth lens has a distance of InTL on the optical axis, half of the maximum viewing angle of the optical imaging system is HAF, and the first lens object The horizontal distance from the coordinate point at 1/2HEP height on the side surface to the imaging plane parallel to the optical axis is ETL, and the coordinate point at 1/2HEP height on the object side of the first lens to 1 on the image side surface of the fourth lens The horizontal distance between the coordinate points of /2HEP height parallel to the optical axis is EIN, which meets the following conditions: 1.0≦f/HEP≦10.0; 0deg<HAF≦150deg and 0.2≦EIN/ETL<1.

The thickness of a single lens at the height of 1/2 entrance pupil diameter (HEP) particularly affects the correction aberrations of the common area of the field of view of each light within the range of 1/2 entrance pupil diameter (HEP) and the optical path difference between the rays of each field of view The greater the thickness, the better the ability to correct aberrations. However, it will also increase the difficulty of manufacturing. Therefore, it is necessary to control the thickness of a single lens at 1/2 entrance pupil diameter (HEP) height, especially the The ratio of the thickness (ETP) of the 1/2 entrance pupil diameter (HEP) height and the thickness (TP) of the lens on the optical axis (ETP/TP) to which the surface belongs. For example, the thickness of the first lens at 1/2 entrance pupil diameter (HEP) height is represented by ETP1. The thickness of the second lens at 1/2 entrance pupil diameter (HEP) height is represented by ETP2. The remaining lenses in the optical imaging system are at 1/2 entrance pupil The thickness of the diameter (HEP) height, and the way it is expressed by analogy. The sum of the aforementioned ETP1 to ETP4 is SETP, and the embodiment of this creation can satisfy the following formula: 0.3≦SETP/EIN<1.

In order to balance the ability to correct aberrations and reduce the difficulty in manufacturing, it is particularly necessary to control the thickness (ETP) of the lens at 1/2 entrance pupil diameter (HEP) height and the thickness of the lens on the optical axis (TP). ) The proportional relationship between (ETP/TP). For example, the thickness of the first lens at 1/2 entrance pupil diameter (HEP) height is represented by ETP1, the thickness of the first lens on the optical axis is TP1, and the ratio between the two is ETP1/TP1. The thickness of the second lens at 1/2 entrance pupil diameter (HEP) height is represented by ETP2, the thickness of the second lens on the optical axis is TP2, and the ratio between the two is ETP2/TP2. The proportional relationship between the thickness of the remaining lenses in the optical imaging system at 1/2 entrance pupil diameter (HEP) height and the thickness (TP) of the lens on the optical axis, and the expression method can be deduced by analogy. The embodiment of this creation can satisfy the following formula: 0<ETP/TP≦5.

The horizontal distance between two adjacent lenses at 1/2 entrance pupil diameter (HEP) height is represented by ED. The aforementioned horizontal distance (ED) is parallel to the optical axis of the optical imaging system, and particularly affects the 1/2 entrance pupil diameter (HEP). ) The ability to correct aberrations in the common area of the field of view of each light and the optical path difference between each field of view. The greater the horizontal distance, the possibility of correcting aberrations will increase, but at the same time it will also increase the difficulty of manufacturing Therefore, it is necessary to control the horizontal distance (ED) between two specific adjacent lenses at 1/2 entrance pupil diameter (HEP) height.

In order to balance the improvement of the ability to correct aberrations and the reduction of the difficulty of "scaling" the length of the optical imaging system, it is particularly necessary to control the horizontal distance (ED) between the two adjacent lenses at 1/2 entrance pupil diameter (HEP) height and the The proportional relationship (ED/IN) between the horizontal distance (IN) of two adjacent lenses on the optical axis. For example, the horizontal distance between the first lens and the second lens at 1/2 entrance pupil diameter (HEP) height is represented by ED12, the horizontal distance between the first lens and the second lens on the optical axis is IN12, and the ratio between the two is ED12 /IN12. The horizontal distance between the second lens and the third lens at 1/2 entrance pupil diameter (HEP) height is represented by ED23. The horizontal distance between the second lens and the third lens on the optical axis is IN23, and the ratio between the two is ED23/ IN23. The proportional relationship between the horizontal distance between the other two adjacent lenses at 1/2 entrance pupil diameter (HEP) height and the horizontal distance between the two adjacent lenses on the optical axis in the optical imaging system, and the expression is analogous.

The horizontal distance between the coordinate point on the image side surface of the fourth lens at 1/2HEP and the imaging surface parallel to the optical axis is FBL, and the intersection point of the image side surface of the fourth lens with the optical axis to the The horizontal distance of the imaging plane parallel to the optical axis is BL. The embodiment of the present invention balances the ability to correct aberrations and reserves the accommodation space for other optical elements at the same time, which can satisfy the following formula: 0.1≦EBL/BL≦1.5.

The optical imaging system may further include a filter element located between the fourth lens and the imaging surface, and the image side surface of the fourth lens at a coordinate point of 1/2HEP height to the filter element is parallel to The distance of the optical axis is EIR, and the distance between the intersection of the fourth lens image side and the optical axis and the filter element parallel to the optical axis is PIR. The embodiment of this creation can satisfy the following formula: 0.1≦EIR/PIR≦ 1.1.

The aforementioned optical imaging system can be used with image sensing elements whose diagonal length is less than 1/1.2 inches. The size of the image sensing element is preferably 1/2.3 inches. The pixel size is less than 1.4 micrometers (μm), preferably, the pixel size is less than 1.12 micrometers (μm), and the best is that the pixel size is less than 0.9 micrometers (μm). In addition, the optical imaging system can be applied to image sensing elements with an aspect ratio of 16:9.

The aforementioned optical imaging system can be adapted to the requirements of video recording with more than one million or ten million pixels (for example, 4K2K or UHD, QHD) and has good imaging quality.

When |f1|>f4, the total height of the optical imaging system (HOS; Height of Optic System) can be appropriately shortened to achieve the purpose of miniaturization.

When |f2|+|f3|>|f1|+|f4|, at least one of the second lens to the third 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 lens to the third lens of the present invention has a weak positive refractive power, it can effectively share the positive refractive power of the first lens and avoid unnecessary aberrations from appearing prematurely. On the contrary, if the second lens to the first lens At least one of the three lenses has a weak negative refractive power, and the aberration of the correction system can be fine-tuned.

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

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

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

110, 210, 310, 410, 510, 610: the first lens

112,212,312,412,512,612: side of object

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

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

122,222,322,422,522,622: side of object

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

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

132,232,332,432,532,632: Object side

134,234,334,434,534,634: like profile

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

142,242,342,442,542,642: Object side

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

170, 270, 370, 470, 570, 670: infrared filter

180,280,380,480,580,680: imaging surface

190,290,390,490,590,690: image sensor

f: focal length of optical imaging system

f1, f2, f3, f4: the focal length of the first lens to the fourth lens

f/HEP, Fno, F#: The aperture value of the optical imaging system

HAF: Half of the maximum viewing angle of the optical imaging system

NA1: Dispersion coefficient of the first lens

NA2, NA3, NA4: the dispersion coefficient of the second lens to the fourth lens

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

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

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

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

TP1: The thickness of the first lens on the optical axis

TP2, TP3, TP4: the thickness of the second lens to the fourth lens on the optical axis

ΣTP: the sum of the thickness of all refractive lenses

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

IN23: The separation 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

InRS41: The horizontal displacement distance from the intersection of the object side of the fourth lens on the optical axis to the maximum effective radius position of the object side of the fourth lens on the optical axis

IF411: The inflection point closest to the optical axis on the object side of the fourth lens

SGI411: The amount of subsidence at this point

HIF411: The vertical distance between the inflection point closest to the optical axis on the object side of the fourth lens and the optical axis

IF421: The inflection point closest to the optical axis on the image side of the fourth lens

SGI421: The amount of subsidence at this point

HIF421: The vertical distance between the inflection point closest to the optical axis on the image side of the fourth lens and the optical axis

IF412: The second inflection point close to the optical axis on the object side of the fourth lens

SGI412: The amount of subsidence at this point

HIF412: The vertical distance between the second inflection point on the object side of the fourth lens near the optical axis and the optical axis

IF422: The second inflection point close to the optical axis on the image side of the fourth lens

SGI422: The amount of subsidence at this point

HIF422: The vertical distance between the inflection point of the second near the optical axis of the fourth lens image side and the optical axis

IF413: The third inflection point close to the optical axis on the object side of the fourth lens

SGI413: The amount of subsidence at this point

HIF413: The vertical distance between the inflection point of the third near the optical axis and the optical axis on the object side of the fourth lens

IF423: The third inflection point close to the optical axis on the image side of the fourth lens

SGI423: The amount of subsidence at this point

HIF423: The vertical distance between the inflection point of the third near the optical axis of the fourth lens image side and the optical axis

IF414: The fourth inflection point close to the optical axis on the object side of the fourth lens

SGI414: The amount of subsidence at this point

HIF414: The vertical distance between the inflection point of the fourth lens on the object side of the fourth lens and the optical axis

IF424: The fourth inflection point close to the optical axis on the image side of the fourth lens

SGI424: The amount of subsidence at this point

HIF424: The vertical distance between the inflection point of the fourth lens on the image side of the fourth lens and the optical axis

C41: Critical point of the fourth lens object side

C42: The critical point of the fourth lens image side

SGC41: The horizontal displacement distance between the critical point of the fourth lens object side and the optical axis

SGC42: The horizontal displacement distance between the critical point of the fourth lens image side and the optical axis

HVT41: The vertical distance between the critical point of the fourth lens object side and the optical axis

HVT42: The vertical distance between the critical point of the fourth lens image side and the optical axis

HOS: Total height of the system (the distance from the object side of the first lens to the imaging surface on the optical axis)

Dg: The diagonal length of the image sensor

InS: distance from aperture to imaging surface

InTL: the distance from the object side of the first lens to the image side of the fourth lens

InB: The distance from the side of the fourth lens to the imaging surface

HOI: Half of the diagonal length of the effective sensing area of the image sensor (maximum image height)

TDT: TV distortion of the optical imaging system at the time of image formation (TV Distortion)

ODT: Optical Distortion of the Optical Imaging System during Image Setting (Optical Distortion)

The above and other features of this creation will be described in detail with reference to the accompanying drawings.

Figure 1A is a schematic diagram of the optical imaging system of the first embodiment of this creation; Figure 1B shows the spherical aberration, astigmatism, and optical distortion of the optical imaging system of the first embodiment of this creation in order from left to right Graph; Figure 1C is a diagram showing the visible light spectrum modulation conversion characteristic diagram of the optical imaging system of the first embodiment of this creation; Figure 2A is a schematic diagram of the optical imaging system of the second embodiment of this creation; Figure 2B is from the left To the right, the graphs of spherical aberration, astigmatism, and optical distortion of the optical imaging system of the second embodiment of this creation are drawn in sequence; Figure 2C is a diagram showing the visible light spectrum modulation conversion characteristics of the optical imaging system of the second embodiment of this creation Figure; Figure 3A is a schematic diagram showing the optical imaging system of the third embodiment of this creation; Figure 3B shows the spherical aberration, astigmatism and optics of the optical imaging system of the third embodiment of this creation in order from left to right Distortion curve diagram; Figure 3C is a diagram showing the visible light spectrum modulation conversion characteristic diagram of the optical imaging system of the third embodiment of this creation; Figure 4A is a schematic diagram of the optical imaging system of the fourth embodiment of this creation; Figure 4B From left to right, the graphs of spherical aberration, astigmatism and optical distortion of the optical imaging system of the fourth embodiment of this creation are drawn in order; Figure 4C shows the visible light spectrum modulation of the optical imaging system of the fourth embodiment of this creation Conversion characteristic diagram; Figure 5A is a schematic diagram showing the optical imaging system of the fifth embodiment of this creation; Figure 5B shows the spherical aberration and astigmatism of the optical imaging system of the fifth embodiment of this creation in order from left to right And the curve diagram of optical distortion; Figure 5C is a diagram showing the visible light spectrum modulation conversion characteristic diagram of the optical imaging system of the fifth embodiment of this creation; Figure 6A is a schematic diagram of the optical imaging system of the sixth embodiment of this creation; Figure 6B is drawn from left to right The preface is a graph showing the spherical aberration, astigmatism, and optical distortion of the optical imaging system according to the sixth embodiment of this creation; Figure 6C is a diagram showing the visible light spectrum modulation conversion characteristic diagram of the optical imaging system according to the sixth embodiment of this creation.

An optical imaging system includes a first lens, a second lens, a third lens, and a fourth lens with refractive power in sequence from the object side to the image side. The optical imaging system may further include an image sensing element disposed on the imaging surface.

The optical imaging system can be designed with three working wavelengths, namely 486.1nm, 587.5nm, and 656.2nm, of which 587.5nm is the main reference wavelength and the reference wavelength for the main extraction technology features. The optical imaging system can also be designed with five working wavelengths, which are 470nm, 510nm, 555nm, 610nm, 650nm, of which 555nm is the main 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 ΣPPR, and the sum of NPR of all negative refractive power lenses is ΣNPR. When the following conditions are met, it will help control the total refractive power and total length of the optical imaging system: 0.5≦ΣPPR/｜ΣNPR｜≦4.5, better It can meet the following conditions: 1≦ΣPPR/|ΣNPR|≦3.5.

The system height of the optical imaging system is HOS. When the HOS/f ratio approaches 1, it will be beneficial to make an optical imaging system that is miniaturized and can image ultra-high pixels.

The total focal length fp of each lens with positive refractive power in the optical imaging system is ΣPP, and the total focal length of each lens with negative refractive power is ΣNP. An embodiment of an imaging system that satisfies the following conditions: 0<ΣPP≦200; and f1/ΣPP≦0.85. Preferably, the following conditions can be satisfied: 0<ΣPP≦150; and 0.01≦f1/ΣPP≦0.7. This helps to control the focusing ability of the optical imaging system and appropriately distribute the positive refractive power of the system to suppress the premature occurrence of significant aberrations.

The first lens may have a positive refractive power, and its object side surface may be convex. Thereby, the strength of the positive refractive power of the first lens can be appropriately adjusted, which helps to shorten the total length of the optical imaging system.

The second lens may have negative refractive power. Thereby, the aberration generated by the first lens can be corrected.

The third lens may have positive refractive power. Thereby, the positive refractive power of the first lens can be shared.

The fourth lens may have negative refractive power, and its image side surface may be concave. This helps to shorten the back focal length to maintain miniaturization. In addition, at least one surface of the fourth lens can have at least one inflection point, which can effectively suppress the incident angle of the off-axis view field, and further can correct the aberration of the off-axis view field. Preferably, both the object side and the image side have at least one inflection point.

The optical imaging system may further include an image sensing element disposed on the imaging surface. The half of the diagonal length of the effective sensing area of the image sensor element (that is, the imaging height or maximum image height of the optical imaging system) is HOI, and the distance from the object side of the first lens to the imaging surface on the optical axis is HOS, which Meet the following conditions: HOS/HOI≦3; and 0.5≦HOS/f≦3.0. Preferably, the following conditions can be satisfied: 1≦HOS/HOI≦2.5; and 1≦HOS/f≦2. In this way, the miniaturization of the optical imaging system can be maintained to be mounted on thin and portable electronic products.

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

In the optical imaging system of this creation, the aperture configuration can be a front aperture or a middle aperture. 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 imaging surfaces. If the aperture is a front aperture, the exit pupil of the optical imaging system and the imaging surface can produce a longer distance to accommodate more optical elements, and can increase the efficiency of image sensing elements to receive images; if it is a central aperture, the system It helps to expand the field of view of the system, so that the optical imaging system has the advantage of a wide-angle lens. The distance from the aforementioned aperture to the imaging surface is InS, which satisfies the following conditions: 0.5≦InS/HOS≦1.1. Preferably, the following conditions can be satisfied: 0.8≦InS/HOS≦1, whereby the miniaturization of the optical imaging system and the wide-angle characteristics can be maintained at the same time.

In the optical imaging system of this creation, the distance between the object side of the first lens and the image side of the fourth lens is InTL, and the total thickness of all refractive lenses on the optical axis ΣTP, which meets the following conditions: 0.45≦ΣTP/InTL ≦0.95. Preferably, the following conditions can be satisfied: 0.6≦ΣTP/InTL≦0.9. In this way, the contrast of the system imaging and the yield rate 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 radius of curvature of the object side of the first lens is R1, and the radius of curvature of the image side of the first lens is R2, which satisfies the following conditions: 0.01≦|R1/R2|≦0.5. In this way, the first lens has a proper positive refractive power strength to avoid excessive increase in spherical aberration. Preferably, the following conditions can be satisfied: 0.01≦|R1/R2|≦0.4.

The radius of curvature of the object side of the fourth lens is R7, and the radius of curvature of the image side of the fourth lens is R8, which meets the following conditions: -200<(R7-R8)/(R7+R8)<30. 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 condition: 0<IN12/f≦0.25. Preferably, the following conditions can be satisfied: 0.01≦IN12/f≦0.20. This helps to improve the chromatic aberration of the lens to enhance its performance.

The distance between the second lens and the third lens on the optical axis is IN23, which satisfies the following conditions: 0<IN23/f≦0.25. Preferably, the following conditions can be satisfied: 0.01≦IN23/f≦0.20. This helps to improve the performance of the lens.

The distance between the third lens and the fourth lens on the optical axis is IN34, which satisfies the following conditions: 0<IN34/f≦0.25. Preferably, the following conditions can be satisfied: 0.001≦IN34/f≦0.20. This helps to improve the performance of the lens.

The thicknesses of the first lens and the second lens on the optical axis are respectively TP1 and TP2, which satisfy the following conditions: 1≦(TP1+IN12)/TP2≦10. This helps to control the sensitivity of the optical imaging system manufacturing and improve its performance.

The thickness of the third lens and the fourth lens on the optical axis are TP3 and TP4, respectively. The separation distance between the two lenses on the optical axis is IN34, which satisfies the following condition: 0.2≦(TP4+IN34)/TP4≦3. This helps to control the sensitivity of the optical imaging system manufacturing and reduce the overall height of the system.

The distance between the second lens and the third lens on the optical axis is IN23, and the total distance between the first lens and the fourth lens on the optical axis is ΣTP, which satisfies the following conditions: 0.01≦ IN23/(TP2+IN23+TP3)≦0.5. Preferably, the following conditions can be satisfied: 0.05≦IN23/(TP2+IN23+TP3)≦0.4. This helps to slightly correct the aberrations caused by the incident light traveling process and reduce the overall height of the system.

In the optical imaging system of this creation, the horizontal displacement distance from the intersection of the fourth lens object side surface 142 on the optical axis to the maximum effective radius position of the fourth lens object side surface 142 on the optical axis is InRS41 (if the horizontal displacement faces the image side, InRS41 Is a positive value; if the horizontal displacement is toward the object side, InRS41 is a negative value), the horizontal displacement distance from the intersection of the fourth lens image side surface 144 on the optical axis to the maximum effective radius position of the fourth lens image side surface 144 to the optical axis is InRS42 The thickness of the fourth lens 140 on the optical axis is TP4, which meets the following conditions: -1mm≦InRS41≦1mm; -1mm≦InRS42≦1mm; 1mm≦｜InRS41｜+｜InRS42｜≦2mm; 0.01≦｜InRS41｜ /TP4≦10; 0.01≦｜InRS42｜/TP4≦10. In this way, the position of the maximum effective radius between the two surfaces of the fourth lens can be controlled, which helps correct the aberration of the peripheral field of view of the optical imaging system and effectively maintain its miniaturization.

In the optical imaging system of this creation, the horizontal displacement distance between the intersection of the object side of the fourth lens on the optical axis and the inflection point of the closest optical axis of the object side of the fourth lens parallel to the optical axis is represented by SGI411, and the fourth lens image The horizontal displacement distance parallel to the optical axis from the intersection point of the side surface on the optical axis to the inflection point of the nearest optical axis of the fourth lens image side is expressed in SGI421, which meets the following conditions: 0<SGI411/(SGI411+TP4)≦0.9 ; 0<SGI421/(SGI421+TP4)≦0.9. Preferably, the following conditions can be satisfied: 0.01<SGI411/(SGI411+TP4)≦0.7; 0.01<SGI421/(SGI421+TP4)≦0.7.

The horizontal displacement distance parallel to the optical axis from the intersection of the object side of the fourth lens on the optical axis to the second inflection point on the object side of the fourth lens that is close to the optical axis is represented by SGI412. The image side of the fourth lens is on the optical axis. The horizontal displacement distance parallel to the optical axis from the intersection point to the second inflection point of the fourth lens image side surface close to the optical axis is represented by SGI422, which meets the following conditions: 0<SGI412/(SGI412+TP4)≦0.9; 0<SGI422 /(SGI422+TP4)≦0.9. Preferably, the following conditions can be satisfied: 0.1≦SGI412/(SGI412+TP4)≦0.8; 0.1≦SGI422/(SGI422+TP4)≦0.8.

The vertical distance between the inflection point of the closest optical axis of the fourth lens on the object side and the optical axis is represented by HIF411. The intersection of the image side of the fourth lens on the optical axis to the reflex point of the closest optical axis on the image side of the fourth lens and the optical axis The vertical distance between the two is represented by HIF421, which meets the following conditions: 0.01≦ HIF411/HOI≦0.9; 0.01≦HIF421/HOI≦0.9. Preferably, the following conditions can be satisfied: 0.09≦HIF411/HOI≦0.5; 0.09≦HIF421/HOI≦0.5.

The vertical distance between the reflex point of the second near the optical axis of the fourth lens on the object side and the optical axis is represented by HIF412. The intersection of the image side of the fourth lens on the optical axis to the reflex of the second near the optical axis of the fourth lens image side The vertical distance between the point and the optical axis is represented by HIF422, which satisfies the following conditions: 0.01≦HIF412/HOI≦0.9; 0.01≦HIF422/HOI≦0.9. Preferably, the following conditions can be satisfied: 0.09≦HIF412/HOI≦0.8; 0.09≦HIF422/HOI≦0.8.

The vertical distance between the reflex point of the third near the optical axis of the fourth lens on the object side and the optical axis is represented by HIF413. The intersection of the image side of the fourth lens on the optical axis to the reflex of the third near the optical axis of the fourth lens image side The vertical distance between the point and the optical axis is represented by HIF423, which meets the following conditions: 0.001mm≦|HIF413|≦5mm; 0.001mm≦|HIF423|≦5mm. Preferably, the following conditions can be satisfied: 0.1mm≦|HIF423|≦3.5mm; 0.1mm≦|HIF413|≦3.5mm.

The vertical distance between the reflex point of the fourth near the optical axis of the fourth lens on the object side and the optical axis is represented by HIF414. The intersection of the image side of the fourth lens on the optical axis to the reflex of the fourth near the optical axis on the image side of the fourth lens The vertical distance between the point and the optical axis is represented by HIF424, which meets the following conditions: 0.001mm≦｜HIF414｜≦5mm; 0.001mm≦｜HIF424｜≦5mm. Preferably, the following conditions can be satisfied: 0.1mm≦|HIF424|≦3.5mm; 0.1mm≦|HIF414|≦3.5mm.

An implementation of the optical imaging system created by the present invention can help correct the chromatic aberration of the optical imaging system by staggering lenses with high and low dispersion coefficients.

The equation system of the above aspheric surface is: z=ch ² /[1+[1-(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) Among them, z is the position value referenced by the surface vertex at the height of h along the optical axis, k is the conical surface coefficient, and c is the reciprocal 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 this creation, the material of the lens can be plastic or glass. When the lens material is plastic, the production cost and weight can be effectively reduced. In addition, when the lens material is glass, the thermal effect can be controlled and the design space for the refractive power configuration of the optical imaging system can be increased. In addition, the object side and image side of the first lens to the fourth lens in the optical imaging system can be aspherical, which can obtain more control variables. In addition to reducing aberrations, compared to the use of traditional glass lenses, The number of lenses used can be reduced, so the total height of the optical imaging system of the creative can be effectively reduced.

Furthermore, in the optical imaging system provided by this creation, if the lens surface is convex, it means that the lens surface is convex at the near optical axis; if the lens surface is concave, it means the lens surface is concave at the near optical axis.

In addition, in the optical imaging system of this invention, at least one diaphragm can be set according to requirements to reduce stray light and help improve image quality.

The optical imaging system of this creation can be applied to a mobile focusing optical system based on demand, and has 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, and the driving module can be coupled with the lenses and displace the lenses. The aforementioned driving module may be a voice coil motor (VCM) for driving the lens to focus, or an optical anti-vibration element (OIS) for reducing the frequency of out-of-focus caused by lens vibration during shooting.

The optical imaging system of the present invention can also make at least one of the first lens, the second lens, the third lens, and the fourth lens a light filtering element with a wavelength of less than 500nm, which can be used with the specific filtering function. At least one surface of the lens is coated with a film or the lens itself is made of a material that can filter out short wavelengths.

The imaging surface of the optical imaging system of this creation can be selected as a flat surface or a curved surface according to requirements. When the imaging surface is a curved surface (for example, a spherical surface with a radius of curvature), it helps to reduce the incident angle required to focus the light on the imaging surface. In addition to helping to achieve the length of the miniature optical imaging system (TTL), it also helps to improve the relative The illuminance also helps.

According to the above-mentioned embodiments, specific examples are presented below and described in detail in conjunction with the drawings.

First embodiment

Please refer to Figures 1A to 1C. Figure 1A shows a schematic diagram of an optical imaging system according to the first embodiment of the invention. Figure 1B shows the optical imaging system of the first embodiment in order from left to right. Graphs of spherical aberration, astigmatism and optical distortion. Figure 1C is a visible light modulation conversion characteristic diagram of the optical imaging system of the first embodiment. It can be seen from Figure 1A that the optical imaging system 10 is from the object side to The image side sequentially includes an aperture 100, a first lens 110, a second lens 120, a third lens 130, a fourth lens 140, an infrared filter 170, an imaging surface 180, and an image sensor 190.

The first lens 110 has a positive refractive power and is made of plastic material. Its object side surface 112 is convex, its image side surface 114 is concave, and both are aspherical, and its object side 112 and image side 114 both have a point of inflection. The thickness of the first lens on the optical axis is TP1, and the thickness of the first lens at 1/2 entrance pupil diameter (HEP) height is represented by ETP1.

The horizontal displacement distance parallel to the optical axis from the intersection point of the object side surface of the first lens on the optical axis to the inflection point of the closest optical axis of the object side surface of the first lens is represented by SGI111, and the intersection point of the image side surface of the first lens on the optical axis to The horizontal displacement distance between the inflection point of the closest optical axis of the first lens image side and the optical axis parallel to the optical axis is represented by SGI121, which meets the following conditions: SGI111=0.2008mm; SGI121=0.0113mm;|SGI111|/(|SGI111|+ TP1)=0.3018; |SGI121|/(|SGI121|+TP1)=0.0238.

The vertical distance between the point of intersection of the object side of the first lens on the optical axis and the inflection point of the closest optical axis of the object side of the first lens to the optical axis is represented by HIF111. The intersection of the image side of the first lens on the optical axis to the first transparent The vertical distance between the inflection point of the closest optical axis on the mirror side and the optical axis is represented by HIF121, which meets the following conditions: HIF111=0.7488mm; HIF121=0.4451mm; HIF111/HOI=0.2552; HIF121/HOI=0.1517.

The second lens 120 has a positive refractive power and is made of plastic material. Its object side 122 is concave, its image side 124 is convex, and both are aspherical, and its object side 122 has an inflection point. The thickness of the second lens on the optical axis is TP2, and the thickness of the second lens at 1/2 entrance pupil diameter (HEP) height is represented by ETP2.

The horizontal displacement distance parallel to the optical axis between the intersection point of the second lens object side surface on the optical axis and the closest optical axis inflection point of the second lens object side surface is represented by SGI211, and the intersection point of the second lens image side surface on the optical axis to The horizontal displacement distance between the inflection point of the closest optical axis of the second lens image side and the optical axis parallel to the optical axis is represented by SGI221, which meets the following conditions: SGI211=-0.1791mm; |SGI211|/(|SGI211|+TP2)=0.3109 .

The vertical distance between the intersection of the object side surface of the second lens on the optical axis and the inflection point of the closest optical axis of the object side of the second lens and the optical axis is represented by HIF211. The vertical distance between the inflection point of the closest optical axis on the mirror side and the optical axis is represented by HIF221, which meets the following conditions: HIF211=0.8147mm; HIF211/HOI=0.2777.

The third lens 130 has a negative refractive power and is made of plastic. Its object side surface 132 is concave, its image side surface 134 is convex, and both are aspherical, and its image side surface 134 has an inflection point. The thickness of the third lens on the optical axis is TP3, and the thickness of the third lens at 1/2 entrance pupil diameter (HEP) height is represented by ETP3.

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 inflection point of the closest optical axis of the object side of the third lens is represented by SGI311, and the intersection of the image side of the third lens on the optical axis to The horizontal displacement distance between the inflection point of the closest optical axis of the third lens image side and the optical axis parallel to the optical axis is represented by SGI321, which meets the following conditions: SGI321=-0.1647mm; |SGI321|/(|SGI321|+TP3)=0.1884 .

The vertical distance between the inflection point of the closest optical axis on the object side of the third lens and the optical axis is represented by HIF311. The intersection point of the image side of the third lens on the optical axis to the inflection point of the closest optical axis on the image side of the third lens and the optical axis The vertical distance between the two is represented by HIF321, which meets the following conditions: HIF321=0.7269mm; HIF321/HOI=0.2477.

The fourth lens 140 has a negative refractive power and is made of plastic. Its object side surface 142 is convex, its image side surface 144 is concave, and both are aspherical, and its object side surface 142 has two inflection points and the image side surface 144 has one Recurve point. The thickness of the fourth lens on the optical axis is TP4, and the thickness of the fourth lens at 1/2 entrance pupil diameter (HEP) height is represented by ETP4.

The horizontal displacement distance parallel to the optical axis from the intersection of the object side of the fourth lens on the optical axis to the inflection point of the closest optical axis of the object side of the fourth lens is represented by SGI411, and the intersection of the image side of the fourth lens on the optical axis to The horizontal displacement distance between the inflection point of the nearest optical axis of the fourth lens image side and the optical axis parallel to the optical axis is represented by SGI421, which meets the following conditions: SGI411=0.0137mm; SGI421=0.0922mm; |SGI411|/(|SGI411|+ TP4)=0.0155; |SGI421|/(|SGI421|+TP4)=0.0956.

The horizontal displacement distance parallel to the optical axis from the intersection of the object side of the fourth lens on the optical axis to the second inflection point of the object side of the fourth lens near the optical axis is represented by SGI412, which satisfies the following conditions: SGI412=-0.1518mm ;|SGI412|/(|SGI412|+TP4)=0.1482.

The vertical distance between the reflex point of the closest optical axis on the object side of the fourth lens and the optical axis is represented by HIF411, and the vertical distance between the reflex point of the closest optical axis on the image side of the fourth lens and the optical axis is represented by HIF411, which meets the following conditions : HIF411=0.2890mm; HIF421=0.5794mm; HIF411/HOI=0.0985; HIF421/HOI=0.1975.

The vertical distance between the reflex point of the second near optical axis on the object side of the fourth lens and the optical axis is represented by HIF412, which meets the following conditions: HIF412=1.3328mm; HIF412/HOI=0.4543.

The distance from the coordinate point on the object side of the first lens at 1/2HEP height to the imaging plane parallel to the optical axis is ETL, and the coordinate point on the object side of the first lens at 1/2HEP height to the image side of the fourth lens The horizontal distance parallel to the optical axis between the coordinate points of 1/2HEP height is EIN, which meets the following conditions: ETL=18.744mm; EIN=12.339mm; EIN/ETL=0.658.

This embodiment meets the following conditions: ETP1=0.949mm; ETP2=2.483mm; ETP3=0.345mm; ETP4=1.168mm. The sum of the aforementioned ETP1 to ETP4 SETP=4.945mm. TP1=0.918mm; TP2=2.500mm; TP3=0.300mm; TP4=1.248mm; the sum of the aforementioned TP1 to TP4 STP=4.966mm; SETP/STP=0.996.

This embodiment specifically controls the proportional relationship (ETP/TP) between the thickness (ETP) of each lens at 1/2 entrance pupil diameter (HEP) height and the thickness (TP) of the lens on the optical axis to which the surface belongs. , In order to strike a balance between manufacturability and aberration correction capability, it satisfies the following conditions, ETP1/TP1=1.034; ETP2/TP2=0.993; ETP3/TP3=1.148; ETP4/TP4=0.936.

This embodiment is to control the horizontal distance of each adjacent two lenses at 1/2 entrance pupil diameter (HEP) height to achieve a balance between the length of the optical imaging system, the degree of "shrinkage", the manufacturability and the ability to correct aberrations. , Especially to control the proportional relationship between the horizontal distance (ED) of the two adjacent lenses at 1/2 entrance pupil diameter (HEP) height and the horizontal distance (IN) of the two adjacent lenses on the optical axis (ED/IN) ), which meets the following conditions, the horizontal distance between the first lens and the second lens at 1/2 entrance pupil diameter (HEP) height parallel to the optical axis is ED12=4.529mm; the second lens and the third lens are between 1 The horizontal distance between /2 entrance pupil diameter (HEP) height parallel to the optical axis is ED23=2.735mm; the horizontal distance between the third lens and the fourth lens at 1/2 entrance pupil diameter (HEP) height parallel to the optical axis It is ED34=0.131mm.

The horizontal distance between the first lens and the second lens on the optical axis is IN12=4.571mm, and the ratio between the two is ED12/IN12=0.991. The horizontal distance between the second lens and the third lens on the optical axis is IN23=2.752mm, and the ratio between the two is ED23/IN23=0.994. The horizontal distance between the third lens and the fourth lens on the optical axis is IN34=0.094mm, and the ratio between the two is ED34/IN34=1.387.

The horizontal distance from the coordinate point on the image side surface of the fourth lens at 1/2HEP to the imaging surface parallel to the optical axis is EBL=6.405mm, and the intersection point on the image side surface of the fourth lens with the optical axis The horizontal distance from the imaging surface parallel to the optical axis is BL=6.3642mm, and the embodiment of this creation can satisfy the following formula: EBL/BL=1.00641. In this embodiment, the distance between the coordinate point at 1/2HEP height on the side of the fourth lens image and the infrared filter parallel to the optical axis is EIR=0.065mm, and the intersection point on the side of the fourth lens image with the optical axis to the infrared filter The distance between the light sheets parallel to the optical axis is PIR=0.025mm, and satisfies the following formula: EIR/PIR=2.631.

The infrared filter 170 is made of glass, which is disposed between the fourth lens 140 and the imaging surface 180 and does not affect the focal length of the optical imaging system.

In the optical imaging system of the first embodiment, the focal length of the optical imaging system is f, the entrance pupil diameter of the optical imaging system is HEP, and half of the maximum viewing angle in the optical imaging system is HAF, and its value is as follows: f=3.4375mm; f/ HEP=2.23; and HAF=39.69 degrees and tan(HAF)=0.8299.

In the optical imaging system of the first embodiment, the focal length of the first lens 110 is f1, and the focal length of the fourth lens 140 is f4, which meets the following conditions: f1=3.2736mm; |f/f1|=1.0501; f4=-8.3381 mm; and |f1/f4|=0.3926.

In the optical imaging system of the first embodiment, the focal lengths of the second lens 120 to the third lens 130 are respectively f2 and f3, which satisfy the following conditions: |f2|+|f3|=10.0976mm;|f1|+|f4| =11.6116mm and |f2|+|f3|<|f1|+|f4|.

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, the optics of the first embodiment In the imaging system, the total PPR of all lenses with positive refractive power is ΣPPR=｜f/f1｜+｜f/f2｜=1.95585, and the total NPR of all lenses with negative refractive power is ΣNPR=｜f/f3｜+｜f /f4｜=0.95770, ΣPPR/｜ΣNPR｜=2.04224. At the same time, the following conditions are also satisfied: |f/f1|=1.05009; |f/f2|=0.90576; |f/f3|=0.54543; |f/f4|=0.41227.

In the optical imaging system of the first embodiment, the distance between the object side 112 of the first lens and the image side 144 of the fourth lens is InTL, the distance between the object side 112 of the first lens and the imaging surface 180 is HOS, and the aperture is 100 to the imaging surface. The distance between 180 is InS, half of the diagonal length of the effective sensing area of the image sensor 190 is HOI, and the distance between the image side surface 144 of the fourth lens and the imaging surface 180 is InB, which satisfies the following conditions: InTL+InB= HOS; HOS=4.4250mm; HOI=2.9340mm; HOS/HOI=1.5082; HOS/f=1.2873; InTL/HOS=0.7191; InS=4.2128mm; and InS/HOS=0.95204.

In the optical imaging system of the first embodiment, the total thickness of all refractive lenses on the optical axis is ΣTP, which meets the following conditions: ΣTP=2.4437 mm; and ΣTP/InTL=0.76793. In this way, the contrast of the system imaging and the yield rate 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 the first embodiment, the curvature radius of the first lens object side 112 is R1, and the curvature radius of the first lens image side 114 is R2, which meets the following conditions: |R1/R2|=0.1853. In this way, the first lens has a proper positive refractive power strength to avoid excessive increase in spherical aberration.

In the optical imaging system of the first embodiment, the curvature radius of the fourth lens object side surface 142 is R7, and the curvature radius of the fourth lens image side surface 144 is R8, which meets the following conditions: (R7-R8)/(R7+R8) =0.2756. This is beneficial to correct the astigmatism generated by the optical imaging system.

In the optical imaging system of the first embodiment, the individual focal lengths of the first lens 110 and the second lens 120 are f1 and f2 respectively, and the sum of the focal lengths of all lenses with positive refractive power is ΣPP, which satisfies the following conditions: ΣPP=f1+ f2=7.0688mm; and f1/(f1+f2)=0.4631. This helps to appropriately distribute the positive refractive power of the first lens 110 to other positive lenses, so as to suppress the generation of significant aberrations in the course of the incident light rays.

In the optical imaging system of the first embodiment, the individual focal lengths of the third lens 130 and the fourth lens 140 are f3 and f4, respectively, and the sum of the focal lengths of all lenses with negative refractive power is ΣNP, which satisfies the following condition: ΣNP=f3+ f4=-14.6405mm; and f4/(f2+f4)=0.5695. This helps to appropriately distribute the negative refractive power of the fourth lens to other negative lenses, so as to suppress the generation of significant aberrations in the progress of the incident light.

In the optical imaging system of the first embodiment, the separation distance between the first lens 110 and the second lens 120 on the optical axis is IN12, which satisfies the following conditions: IN12=0.3817mm; IN12/f=0.11105. This helps to improve the chromatic aberration of the lens to enhance its performance.

In the optical imaging system of the first embodiment, the separation distance between the second lens 120 and the third lens 130 on the optical axis is IN23, which meets the following conditions: IN23=0.0704mm; IN23/f=0.02048. This helps to improve the chromatic aberration of the lens to enhance its performance.

In the optical imaging system of the first embodiment, the distance between the third lens 130 and the fourth lens 140 on the optical axis is IN34, which satisfies the following conditions: IN34=0.2863mm; IN34/f=0.08330. This helps to improve the chromatic aberration of the lens to enhance its performance.

In the optical imaging system of the first embodiment, the thicknesses of the first lens 110 and the second lens 120 on the optical axis are respectively TP1 and TP2, which satisfy the following conditions: TP1=0.46442mm; TP2=0.39686mm; TP1/TP2= 1.17023 and (TP1+IN12)/TP2=2.13213. This helps to control the sensitivity of the optical imaging system manufacturing and improve its performance.

In the optical imaging system of the first embodiment, the thicknesses of the third lens 130 and the fourth lens 140 on the optical axis are TP3 and TP4, respectively, and the separation distance between the two lenses on the optical axis is IN34, which meets the following conditions: TP3 =0.70989mm; TP4=0.87253mm; TP3/TP4=0.81359 and (TP4+IN34)/TP3=1.63248. This helps to control the sensitivity of the optical imaging system manufacturing and reduce the overall height of the system.

In the optical imaging system of the first embodiment, it satisfies the following condition: IN23/(TP2+IN23+TP3)=0.05980. This helps to slightly correct the aberrations caused by the incident light traveling process and reduce the overall height of the system.

In the optical imaging system of the first embodiment, the horizontal displacement distance from the intersection of the fourth lens object side surface 142 on the optical axis to the maximum effective radius position of the fourth lens object side surface 142 on the optical axis is InRS41, and the fourth lens image side surface 144 The horizontal displacement distance from the intersection on the optical axis to the maximum effective radius position of the image side surface 144 of the fourth lens on the optical axis is InRS42, and the thickness of the fourth lens 140 on the optical axis is TP4, which satisfies the following conditions: InRS41=-0.23761 mm; InRS42=-0.20206mm; |InRS41|+|InRS42|=0.43967mm; |InRS41|/TP4=0.27232; and |InRS42|/TP4=0.23158. This facilitates the production and molding of the lens, and effectively maintains its miniaturization.

In the optical imaging system of this embodiment, the vertical distance between the critical point C41 of the fourth lens object side surface 142 and the optical axis is HVT41, and the vertical distance between the critical point C42 of the fourth lens image side surface 144 and the optical axis is HVT42, which satisfies the following Conditions: HVT41=0.5695mm; HVT42=1.3556mm; HVT41/HVT42=0.4201. In this way, the aberration of the off-axis field of view can be effectively corrected.

The optical imaging system of this embodiment satisfies the following conditions: HVT42/HOI=0.4620. This helps to correct the aberration of the peripheral field of view of the optical imaging system.

The optical imaging system of this embodiment satisfies the following conditions: HVT42/HOS=0.3063. This helps to correct the aberration of the peripheral field of view of the optical imaging system.

In the optical imaging system of the first embodiment, the dispersion coefficient of the first lens is NA1, the dispersion coefficient of the second lens is NA2, the dispersion coefficient of the third lens is NA3, and the dispersion coefficient of the fourth lens is NA4, which satisfies the following conditions : |NA1-NA2|=0; NA3/NA2=0.39921. This helps correct the chromatic aberration of the optical imaging system.

In the optical imaging system of the first embodiment, the optical imaging system is

TV distortion becomes TDT, and the optical distortion at the time of image formation becomes ODT, which meets the following conditions: |TDT|=0.4%; |ODT|=2.5%.

In the optical imaging system of this embodiment, the modulation conversion contrast transfer ratio (MTF value) of the optical axis, 0.3HOI, and 0.7HOI at the half-frequency on the imaging plane is represented by MTFH0, MTFH3, and MTFH7, respectively, which meet the following conditions : MTFH0 is about 0.525; MTFH3 is about 0.375; and MTFH7 is about 0.35.

Refer to Table 1 and Table 2 below for cooperation.

Table 1 is the detailed structure data of the first embodiment, in which the unit of curvature radius, thickness, distance and focal length is mm, and surface 0-14 indicates the surface from the object side to the image side in sequence. Table 2 is the aspheric surface data in the first embodiment, where k represents the conical surface coefficient in the aspheric curve equation, and A1-A20 represent the 1-20th order aspheric surface coefficients of each surface. In addition, the following embodiment tables correspond to the schematic diagrams and aberration curve diagrams of the respective embodiments, and the definitions of the data in the tables are the same as those in Table 1 and Table 2 of the first embodiment, and will not be repeated here.

Second embodiment

Please refer to Figures 2A to 2C, where Figure 2A shows an example of the second embodiment of the present creation A schematic diagram of an optical imaging system. Figure 2B shows the spherical aberration, astigmatism and optical distortion curves of the optical imaging system of the second embodiment in order from left to right. Figure 2C is a visible light spectrum modulation conversion characteristic diagram of the optical imaging system of the second embodiment. As shown in Figure 2A, the optical imaging system 20 includes a first lens 210, an aperture 200, a second lens 220, a third lens 230, a fourth lens 240, an infrared filter 270, and an imaging surface in sequence from the object side to the image side. 280 and image sensor 290.

The first lens 210 has a negative refractive power and is made of glass. Its object side surface 212 is a concave surface, its image side surface 214 is a concave surface, and both are aspherical, and its object side surface 212 has an inflection point.

The second lens 220 has a positive refractive power and is made of glass. Its object side surface 222 is a convex surface, its image side surface 224 is a concave surface, both of which are aspherical surfaces, and its object side surface 222 has an inflection point.

The third lens 230 has a positive refractive power and is made of glass. Its object side surface 232 is convex, its image side surface 234 is convex, and both are aspherical, and its object side surface 232 has an inflection point.

The fourth lens 240 has a negative refractive power and is made of glass. Its object side surface 242 is a convex surface, its image side surface 244 is a concave surface, both of which are aspherical surfaces, and its object side surface 242 has an inflection point.

The infrared filter 270 is made of glass, which is disposed between the fourth lens 240 and the imaging surface 280 and does not affect the focal length of the optical imaging system.

Please refer to Table 3 and Table 4 below for cooperation.

In the second embodiment, the curve equation of the aspheric surface is expressed as in 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 values can be obtained:

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

According to Table 3 and Table 4, the relevant value of the profile curve length can be obtained:

The third embodiment

Please refer to Figures 3A to 3C. Figure 3A shows a schematic diagram of an optical imaging system according to the third embodiment of the present invention. Figure 3B shows the optical imaging system of the third embodiment in order from left to right. Graphs of spherical aberration, astigmatism and optical distortion. Fig. 3C is a characteristic diagram of the visible light spectrum modulation conversion of the optical imaging system of the third embodiment. As shown in Figure 3A, the optical imaging system 30 includes a first lens 310, an aperture 300, a second lens 320, a third lens 330, a fourth lens 340, an infrared filter 370, and an imaging surface in sequence from the object side to the image side. 380 and an image sensor 390.

The first lens 310 has a negative refractive power and is made of plastic. Its object side surface 312 is concave, its image side surface 314 is convex, and both are aspherical, and its object side surface 312 and image side surface 314 have two inflection points.

The second lens 320 has a positive refractive power and is made of plastic material. Its object side surface 322 is a concave surface, and its image side surface 324 is a convex surface, and both are aspherical.

The third lens 330 has positive refractive power and is made of plastic material. Its object side surface 332 is concave, its image side surface 334 is convex, and both are aspherical, and its object side surface 332 and image side surface 334 both have an inflection point.

The fourth lens 340 has negative refractive power and is made of plastic. Its object side surface 342 is concave, its image side surface 344 is concave, and both are aspherical, and its object side surface 332 has an inflection point and the image side surface 334 has two Recurve point.

The infrared filter 370 is made of glass, which is disposed between the fourth lens 340 and the imaging surface 380 and does not affect the focal length of the optical imaging system.

Please refer to Table 5 and Table 6 below for cooperation.

In the third embodiment, the curve equation of the aspheric surface is expressed as in 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 values can be obtained:

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

Fourth embodiment

Please refer to FIG. 4A to FIG. 4C, where FIG. 4A shows an example of the fourth embodiment of the present creation. A schematic diagram of an optical imaging system. Figure 4B shows the spherical aberration, astigmatism, and optical distortion curves of the optical imaging system of the fourth embodiment in order from left to right. Fig. 4C is a characteristic diagram of visible light spectrum modulation conversion of the optical imaging system of the fourth embodiment. It can be seen from Figure 4A that the optical imaging system 40 includes a first lens 410, an aperture 400, a second lens 420, a third lens 430, a fourth lens 440, an infrared filter 470, and an imaging surface in sequence from the object side to the image side. 480 and image sensor 490.

The first lens 410 has a negative refractive power and is made of plastic material. Its object side surface 412 is concave, its image side surface 414 is concave, and both are aspherical, and its object side surface 412 has an inflection point.

The second lens 420 has a positive refractive power and is made of plastic material. Its object side surface 422 is convex, its image side surface 424 is convex, and both are aspherical, and its object side surface 422 has an inflection point.

The third lens 430 has a positive refractive power and is made of plastic material. Its object side surface 432 is a convex surface, its image side surface 434 is a concave surface, and both are aspherical surfaces, and its object side surface 432 has an inflection point.

The fourth lens 440 has a negative refractive power and is made of plastic material. Its object side surface 442 is a concave surface, its image side surface 444 is a convex surface, and both are aspherical, and its image side surface 444 has an inflection point.

The infrared filter 470 is made of glass, which is disposed between the fourth lens 440 and the imaging surface 480 and does not affect the focal length of the optical imaging system.

Please refer to Table 7 and Table 8 below for cooperation.

In the fourth embodiment, the curve equation of the aspheric surface is expressed as in 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 values can be obtained:

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

Fifth embodiment

Please refer to FIGS. 5A to 5C, where FIG. 5A shows a schematic diagram of an optical imaging system according to the fifth embodiment of the present invention, and FIG. 5B shows the optical imaging system of the fifth embodiment in order from left to right. Graphs of spherical aberration, astigmatism and optical distortion. Fig. 5C is a characteristic diagram of visible light spectrum modulation conversion of the optical imaging system of the fifth embodiment. It can be seen from FIG. 5A that the optical imaging system 50 includes a first lens 510, an aperture 500, a second lens 520, a third lens 530, a fourth lens 540, an infrared filter 570, and an imaging surface in sequence from the object side to the image side. 580 and image sensor 590.

The first lens 510 has a negative refractive power and is made of plastic. Its object side surface 512 is convex, its image side surface 514 is concave, and both are aspherical, and its object side surface 512 and image side surface 314 both have an inflection point.

The second lens 520 has a positive refractive power and is made of plastic material. Its object side surface 522 is a convex surface, its image side surface 524 is a concave surface, and both are aspherical surfaces, and its object side surface 522 has an inflection point.

The third lens 530 has a positive refractive power and is made of plastic material. Its object side surface 532 is convex, and its image side surface 534 is convex, both of which are aspherical, and its object side surface 532 has two inflection points.

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

The infrared filter 570 is made of glass, which is disposed between the fourth lens 540 and the imaging surface 580 and does not affect the focal length of the optical imaging system.

Please refer to Table 9 and Table 10 below for cooperation.

In the fifth embodiment, the aspherical curve equation is expressed as in 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 values can be obtained:

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

Sixth embodiment

Please refer to FIGS. 6A to 6C, where FIG. 6A shows a schematic diagram of an optical imaging system according to the sixth embodiment of the present creation, and FIG. 6B shows the optical imaging system of the sixth embodiment in order from left to right. Graphs of spherical aberration, astigmatism and optical distortion. Fig. 6C is a characteristic diagram of visible light spectrum modulation conversion of the optical imaging system of the sixth embodiment. It can be seen from FIG. 6A that the optical imaging system 60 includes a first lens 610, an aperture 600, a second lens 620, a third lens 630, a fourth lens 640, an infrared filter 670, and an imaging surface in sequence from the object side to the image side. 680 and image sensor 690.

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

The second lens 620 has a positive refractive power and is made of plastic material. Its object side surface 622 is a convex surface, its image side surface 624 is a convex surface, and both are aspherical, and its object side surface 622 has an inflection point.

The third lens 630 has positive refractive power and is made of plastic. Its object side surface 632 is concave, its image side surface 634 is convex, and both are aspherical, and its object side surface 632 and image side surface 634 both have an inflection point.

The fourth lens 640 has a negative refractive power and is made of plastic. Its object side surface 642 is convex, its image side surface 644 is concave, and both are aspherical, and its object side surface 632 has an inflection point and the image side surface 634 has two Recurve point.

The infrared filter 670 is made of glass, which is disposed between the fourth lens 640 and the imaging surface 680 and does not affect the focal length of the optical imaging system.

Please refer to Table 11 and Table 12 below for cooperation.

In the sixth embodiment, the curve equation of the aspheric surface is expressed as in 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 values can be obtained:

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

Although this creation has been disclosed in the implementation manner as above, it is not used to limit this creation. Anyone who is familiar with this art can do various things without departing from the spirit and scope of this creation. Therefore, the scope of protection of this creation shall be subject to the scope of the attached patent application.

Although this creation has been specifically shown and described with reference to its exemplary embodiments, it will be understood by those with ordinary knowledge in the technical field that it does not deviate from the spirit of this creation defined by the scope of the patent application and its equivalents below Various changes in form and details can be made under the category and category.

20: Optical imaging system

200: aperture

210: first lens

212: Object side

214: like side

220: second lens

222: Object side

224: like side

230: third lens

232: Object side

234: like side

240: fourth lens

242: Object Side

244: like side

270: Infrared filter

280: imaging surface

290: Image sensor

Claims (25)

An optical imaging system, from the object side to the image side, sequentially includes: a first lens with negative refractive power, the object side surface is concave on the optical axis and has at least one inflection point; a second lens with refractive power A third lens with positive refractive power, and its object side surface is concave on the optical axis; a fourth lens with refractive power; and an imaging surface; wherein the optical imaging system has four refractive power lenses, the At least one of the second lens and the fourth lens has positive refractive power, the focal lengths of the first lens to the fourth lens are f1, f2, f3, and f4, respectively, the focal length of the optical imaging system is f, and the optical imaging The entrance pupil diameter of the system is HEP, the first lens object side to the imaging surface has a distance HOS on the optical axis, the first lens object side to the fourth lens image side has a distance of InTL on the optical axis, the Half of the maximum viewing angle of the optical imaging system is HAF. The thicknesses of the first lens, the second lens, the third lens, and the fourth lens at the height of 1/2HEP and parallel to the optical axis are ETP1, ETP2, and ETP3, respectively And ETP4, the sum of the foregoing ETP1 to ETP4 is SETP, the thickness of the first lens, the second lens, the third lens, and the fourth lens on the optical axis are TP1, TP2, TP3, and TP4, respectively, and the foregoing TP1 to TP4 The sum of is STP, which meets the following conditions: 1.8≦f/HEP≦2.8; 45deg<HAF≦80deg and 0.5≦SETP/STP<1. The optical imaging system according to claim 1, wherein the horizontal distance between the coordinate point at 1/2HEP height on the object side of the first lens and the imaging surface parallel to the optical axis is ETL, and the first lens is on the object side The horizontal distance between the coordinate point of 1/2HEP height and the coordinate point of 1/2HEP height on the image side of the fourth lens parallel to the optical axis is EIN, which satisfies the following condition: 0.2≦EIN/ETL<1. The optical imaging system of claim 2, wherein the thickness of the first lens at a height of 1/2HEP and parallel to the optical axis is ETP1, and the thickness of the second lens at a height of 1/2HEP and parallel to the optical axis is ETP2, The thickness of the third lens at the height of 1/2HEP and parallel to the optical axis is ETP3, the thickness of the fourth lens at the height of 1/2HEP and parallel to the optical axis is ETP4, and the sum of the aforementioned ETP1 to ETP4 is SETP, which satisfies the following Formula: 0.3≦SETP/EIN<1. The optical imaging system according to claim 1, wherein the second lens has a positive refractive power and the object side surface is concave on the optical axis. The optical imaging system according to claim 4, wherein the image side surface of the first lens is convex on the optical axis and the image side surface of the second lens is convex on the optical axis. The optical imaging system according to claim 1, wherein the image side surface of the third lens is convex on the optical axis. The optical imaging system according to claim 1, wherein the object side surface and the image side surface of the fourth lens are both convex on the optical axis. The optical imaging system of claim 1, wherein the imaging height of the optical imaging system is HOI, the optical axis of visible light on the imaging plane, 0.3HOI and 0.7HOI are three modulation conversion contrast transfer rates at a spatial frequency of 55 cycles/mm (MTF value) are represented by MTFE0, MTFE3, and MTFE7 respectively, which meet the following conditions: MTFE0≧0.2; MTFE3≧0.01; and MTFE7≧0.01. The optical imaging system of claim 1, which further includes an aperture, and a distance InS from the aperture to the imaging surface on the optical axis satisfies the following formula: 0.2≦InS/HOS≦1.1. An optical imaging system, from the object side to the image side, sequentially includes: a first lens with negative refractive power, the object side surface is concave on the optical axis and has at least one inflection point; a second lens with refractive power ; A third lens with positive refractive power, and its object side surface is concave on the optical axis and has at least one inflection point; a fourth lens with refractive power; and an imaging surface; wherein the optical imaging system has refractive power There are four lenses in the second lens and the fourth lens at least one lens has a positive refractive power, the focal lengths of the first lens to the fourth lens are f1, f2, f3, f4, and the optical imaging system The focal length is f, the entrance pupil diameter of the optical imaging system is HEP, there is a distance HOS from the object side of the first lens to the imaging surface on the optical axis, and the first lens object There is a distance InTL from the side to the image side of the fourth lens on the optical axis, half of the maximum viewing angle of the optical imaging system is HAF, and between the coordinate point of 1/2HEP on the object side of the first lens and the imaging plane The horizontal distance parallel to the optical axis is ETL, and the horizontal distance between the coordinate point on the object side of the first lens at 1/2HEP height and the coordinate point on the image side of the fourth lens at 1/2HEP height parallel to the optical axis is EIN, which meets the following conditions: 1.8≦f/HEP≦2.8; 45deg<HAF≦80deg and 0.2≦EIN/ETL<1. The optical imaging system according to claim 10, wherein the imaging height of the optical imaging system is HOI, the optical axis of visible light on the imaging plane, 0.3HOI and 0.7HOI are three modulation conversion contrast transfer rates at a spatial frequency of 110 cycles/mm (MTF value) are expressed as MTFQ0, MTFQ3, and MTFQ7 respectively, which meet the following conditions: MTFQ0≧0.2; MTFQ3≧0.01; and MTFQ7≧0.01. The optical imaging system according to claim 10, wherein the optical imaging system satisfies the following formula: 0mm<HOS≦4mm. The optical imaging system of claim 10, wherein the thickness of the second lens at a height of 1/2HEP and parallel to the optical axis is ETP2, and the thickness of the second lens on the optical axis is TP2, which satisfies the following conditions: 0.1 ≦ETP2/TP2≦5. The optical imaging system according to claim 10, wherein the second lens has a positive refractive power and the object side surface is concave on the optical axis. The optical imaging system according to claim 10, wherein the optical imaging system satisfies the following conditions: -3≦f2/f3≦5. The optical imaging system according to claim 10, wherein the optical imaging system satisfies the following condition: f2<f3. The optical imaging system according to claim 10, wherein the optical imaging system satisfies the following conditions: -2≦f1/f4≦3. The optical imaging system according to claim 10, wherein the thicknesses of the second lens and the third lens on the optical axis are TP2 and TP3, respectively, which satisfy the following conditions: 0.1≦TP2/TP3≦10. The optical imaging system according to claim 10, wherein the thicknesses of the second lens and the third lens on the optical axis are TP2 and TP3, respectively, which satisfy the following condition: TP2>TP3. An optical imaging system, from the object side to the image side, sequentially includes: a first lens with negative refractive power, the object side surface is concave on the optical axis, the image side surface is convex on the optical axis, and the object side surface is Each side has at least one inflection point; a second lens has positive refractive power, and its object side is concave on the optical axis; a third lens has positive refractive power, and its object side is concave on the optical axis and has At least one inflection point; a fourth lens with refractive power; and an imaging surface; The optical imaging system has four lenses with refractive power, the focal lengths of the first lens to the fourth lens are f1, f2, f3, and f4, respectively, the focal length of the optical imaging system is f, and the incidence of the optical imaging system The pupil diameter is HEP, the first lens object side to the imaging surface has a distance HOS on the optical axis, the first lens object side to the fourth lens image side has a distance of InTL on the optical axis, the optical imaging system Half of the maximum viewing angle is HAF, the horizontal distance between the coordinate point on the object side of the first lens at 1/2HEP height and the imaging surface parallel to the optical axis is ETL, and the horizontal distance from the object side of the first lens at 1/2HEP The horizontal distance between the height coordinate point and the 1/2HEP height coordinate point on the side of the fourth lens image parallel to the optical axis is EIN, which satisfies the following conditions: 1.8≦f/HEP≦2.8; 45deg<HAF≦80deg and 0.2≦EIN/ETL<1. The optical imaging system according to claim 20, wherein the distance between the third lens and the fourth lens on the optical axis is IN34, and satisfies the following formula: 0<IN34/f≦5. The optical imaging system according to claim 10, wherein the optical imaging system satisfies the following conditions: 0.1≦f2/f3≦5. The optical imaging system according to claim 10, wherein the object side surface and the image side surface of the fourth lens are both concave on the optical axis. The optical imaging system according to claim 20, wherein the image side surface of the fourth lens has at least two inflection points. The optical imaging system of claim 20, wherein the optical imaging system further includes an aperture, an image sensing element, and a driving module Group, the image sensing element is arranged on the imaging surface, and there is a distance InS from the aperture to the imaging mask, the driving module is coupled with the lenses and displaces the lenses, which satisfies the following formula: 0.2 ≦InS/HOS≦1.1.

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