TWM594698U - Optical image capturing system - Google Patents

Abstract

The invention discloses a five-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 refractive power; a second lens with refractive power; a third lens with refractive power; a fourth lens with refractive power; a fifth lens with refractive power; and at least one of the image-side surface and object-side surface of each of the five lens elements is 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 group, and particularly about a miniaturized optical imaging system group applied to electronic products.

In recent years, with the rise of portable electronic products with photographic functions, the demand for optical systems has been increasing. The photosensitive element of the general optical system is nothing more than a photosensitive coupled device (Charge Coupled Device; CCD) or a complementary metal oxide semiconductor device (Complementary Metal-Oxide Semiconductor Sensor; CMOS Sensor), and with the advancement of semiconductor process technology, As a result, the pixel size of the photosensitive element is reduced, and the optical system is gradually developing in the field of high pixels, so the requirements for imaging quality are also increasing.

The traditional optical systems mounted on portable devices mostly use three- or four-piece lens structures. However, as portable devices continue to improve pixels and end consumers demand large apertures such as low light and night With the shooting function, the conventional 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 lens and further improve the imaging quality has become a very important issue.

The aspect of this creative embodiment is directed to an optical imaging system and an optical image capturing lens, which can use the combination of the refractive power of five lenses, convex and concave surfaces (the convex or concave surface in this creation refers to the object side of each lens in principle) Or the description of the change of the geometric shape at different heights from the side of the optical axis, so as to effectively improve the light input of the optical imaging system and improve the imaging quality at the same time, so as to be applied to small electronic products.

The terms and code names of the lens parameters related to this creative example are detailed below, as a reference for subsequent description: lens parameters related to length or height

The imaging height of the optical imaging system is expressed by HOI; the height of the optical imaging system is expressed by HOS; the distance between the object side of the first lens of the optical imaging system and the image side of the fifth lens is expressed by InTL; the fixed diaphragm of the optical imaging system (aperture) ) The distance to 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 (exemplified); the thickness of the first lens of the optical imaging system on the optical axis is represented by TP1 (exemplified) ).

Lens parameters related to materials

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

Lens parameters related to viewing angle

The angle of view is expressed in AF; half of the angle of view is expressed in HAF; the chief ray angle is expressed in MRA.

Lens parameters related to entrance and exit pupils

The diameter of the entrance pupil of the optical imaging system is expressed by HEP; the exit pupil of the optical imaging lens system refers to the image formed by the aperture stop through the lens group behind the aperture stop and formed in the image space, and the exit pupil diameter is expressed by HXP; single The maximum effective radius of any surface of the lens refers to the intersection point (Effective Half Diameter; EHD) of the incident light passing through the outermost edge of the entrance pupil at the maximum viewing angle of the system, and 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 maximum effective radius of any surface of the remaining lenses in the optical imaging system can be expressed by analogy.

Parameters related to the arc length of lens surface and surface profile

The length of the contour curve of the maximum effective radius of any surface of a single lens refers to the lens The intersection of the surface and the optical axis of the associated optical imaging system is the starting point. From the starting point along the surface profile of the lens to the end of its maximum effective radius, the length of the curved arc between the aforementioned two points is the maximum effective radius The length of the contour curve is expressed in ARS. For example, the length of the contour curve of the maximum effective radius of the object side of the first lens is represented by ARS11, and the length of the contour curve of the maximum effective radius of the image side of the first lens is represented by ARS12. The profile curve length of the maximum effective radius of the object side of the second lens is represented by ARS21, and the profile curve length of the maximum effective radius of the image side of the second lens is represented by ARS22. The length of the contour curve of the maximum effective radius of any surface of the remaining lenses in the optical imaging system can be expressed by analogy.

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

Parameters related to the depth of lens profile

From the intersection of the fifth lens object side on the optical axis to the end of the maximum effective radius of the fifth lens object side, the distance between the two points above the optical axis is expressed by InRS51 (maximum effective radius depth); fifth lens image side From the point of intersection on the optical axis to the end of the maximum effective radius of the image side of the fifth lens, the distance between the aforementioned two points horizontally to the optical axis is represented by InRS52 (maximum effective radius depth). The expression of the depth of the maximum effective radius (subsidence amount) of the object side or image side of other lenses is the same as the above.

Parameters related to lens profile

Critical point C refers to a specific lens surface, except for the intersection with the optical axis, one is perpendicular to the optical axis The tangent point. For example, the vertical distance between the critical point C41 on the side of the fourth lens object and the optical axis is HVT41 (exemplified), the vertical distance between the critical point C42 on the image side of the fourth lens and the optical axis is HVT42 (exemplified), and the fifth lens object The vertical distance between the critical point C51 on the side and the optical axis is HVT51 (illustrated), and the vertical distance between the critical point C52 on the image side of the fifth lens and the optical axis is HVT52 (illustrated). The expression method of the critical point on the object side or the image side of other lenses and the vertical distance from the optical axis is as described above.

The inflection point closest to the optical axis on the object side of the fifth lens is IF511, and the amount of depression at this point is SGI511 (exemplified), that is, the intersection point of the object side of the fifth lens on the optical axis to the closest optical axis of the object side of the fifth lens The horizontal displacement distance between the inflexion point and the optical axis is parallel. The vertical distance between the point and the optical axis of IF511 is HIF511 (example). The inflection point closest to the optical axis on the image side of the fifth lens is IF521, and the amount of depression at this point is SGI521 (example), that is, the intersection of the image side of the fifth lens on the optical axis and the closest optical axis of the image side of the fifth lens The horizontal displacement distance between the inflexion point and the optical axis is parallel, and the vertical distance between the point and the optical axis of IF521 is HIF521 (illustrated).

The inflection point of the second lens on the side of the fifth lens close to the optical axis is IF512, and the amount of depression at this point is SGI512 (example), that is, the intersection point of the fifth lens on the optical axis to the second closest to the fifth lens The horizontal displacement distance between the reflex point of the optical axis and the optical axis is parallel. The vertical distance between this point and the optical axis is IF512 (illustrated). The inflection point of the second lens on the image side of the fifth lens close to the optical axis is IF522, and the amount of depression at this point is SGI522 (example), that is, the intersection of the image side of the fifth lens on the optical axis and the second closest to the image side of the fifth lens The horizontal displacement distance between the reflex point of the optical axis and the optical axis is parallel, and the vertical distance between the point and the optical axis of IF522 is HIF522 (illustrated).

The inflection point of the third approaching optical axis on the object side of the fifth lens is IF513, and the amount of depression at this point is SGI513 (example), that is, the intersection of the object side of the fifth lens on the optical axis and the third approaching of the object side of the fifth lens The horizontal displacement distance between the reflex point of the optical axis and the optical axis is parallel, and the vertical distance between this point and the optical axis is HIF513 (illustrated). The third inflection point near the optical axis on the image side of the fifth lens is IF523, and the amount of depression at this point is SGI523 (example), which is the intersection of the image side of the fifth lens on the optical axis and the fifth lens The horizontal displacement distance between the third inflection point close to the optical axis on the image side and the optical axis is parallel. The vertical distance between this point and the optical axis of IF523 is HIF523 (illustrated).

The fourth inflection point on the object side of the fifth lens close to the optical axis is IF514, and the amount of depression at this point is SGI514 (exemplified), that is, the intersection of the object side of the fifth lens on the optical axis and the fourth closest to the object side of the fifth lens The horizontal displacement distance between the reflex point of the optical axis and the optical axis is parallel, and the vertical distance between the point and the optical axis of IF514 is HIF514 (illustrated). The fourth inflection point on the image side of the fifth lens near the optical axis is IF524, and the amount of depression at this point is SGI524 (example), which is the intersection of the image side of the fifth lens on the optical axis to the fourth closest to the image side of the fifth lens The horizontal displacement distance between the reflex point of the optical axis and the optical axis, and the vertical distance between the point and the optical axis of IF524 is HIF524 (illustrated).

The expressions of the inflection points on the object side or image side of other lenses and their vertical distance from the optical axis or the amount of their sinking are the same as those described above.

Variables related to aberrations

The optical distortion of the optical imaging system is expressed by ODT; its TV distortion is expressed by TDT, and it can be further limited to describe the degree of aberration shift between 50% and 100% of the field of view; spherical aberration The shift is expressed in DFS; the comet aberration offset is expressed in DFC.

The lateral aberration of the aperture edge is expressed as STA (STOP Transverse Aberration). To evaluate the performance of a specific optical imaging system, the tangential fan or sagittal fan can be used to calculate the lateral light of any field of view Aberrations, in particular, the lateral aberrations of the longest operating wavelength (for example, 650 NM or 656 NM) and the shortest operating wavelength (for example, 470 NM or 486 NM) through the edge of the aperture are used as the standard for excellent performance. The coordinate direction of the aforementioned meridian plane light fan can be further divided into a positive direction (upper light) and a negative direction (lower light). The longest operating wavelength passes the lateral aberration of the aperture edge, which is defined as the imaging position of the longest operating wavelength incident on the imaging plane at a specific field of view through the aperture edge, which is on the imaging plane with the reference wavelength chief ray (eg, wavelength 555NM or 587.5NM) The difference in the distance between the two imaging positions of the field of view, the shortest operating wavelength passes the lateral aberration of the edge of the aperture, which is defined The shortest operating wavelength is incident on the imaging position of the specific field of view on the imaging plane through the edge of the aperture, and the difference between the position of the reference wavelength chief ray on the imaging plane and the imaging position of the field of view on the imaging plane. The performance of the specific optical imaging system is evaluated as Excellent, the shortest and longest working wavelength can be used as the inspection method when the lateral aberration of the 0.7 field of view (ie 0.7 imaging height HOI) incident on the imaging surface through the aperture edge is less than 20 microns (μm) or 20 pixels (Pixel Size), Even with the shortest and longest working wavelength incident on the imaging plane through the aperture edge, the lateral aberration of 0.7 field of view is less than 10 microns (μm) or 10 pixels (Pixel Size) as the inspection method.

The optical imaging system has a maximum imaging height HOI perpendicular to the optical axis on the imaging plane. The longest operating wavelength of the positive meridian plane fan of the optical imaging system passes through the edge of the entrance pupil and is incident on the imaging plane at the lateral image at 0.7 HOI The difference is expressed in PLTA, and the shortest operating wavelength of the positive meridian plane fan passes the edge of the entrance pupil and is incident on the imaging plane at 0.7HOI. The lateral aberration is expressed in PSTA, and the longest operating wavelength of the negative meridian plane fan passes The lateral aberration of the entrance pupil edge and incident on the imaging plane at 0.7 HOI is expressed as NLTA, and the shortest operating wavelength of the negative meridian plane fan passes through the entrance pupil edge and is incident on the imaging plane at the lateral image of 0.7 HOI The difference is expressed in NSTA. The longest operating wavelength of the sagittal plane fan passes the edge of the entrance pupil and is incident on the imaging plane at 0.7 HOI. The lateral aberration is expressed in SLTA. The shortest operating wavelength of the sagittal plane fan passes the edge of the entrance pupil and The lateral aberration incident on the imaging plane at 0.7 HOI is represented by SSTA.

This creation provides an optical imaging system in which the fifth lens has an inflexion point on the object side or image side, which can effectively adjust the angle of incidence of each field of view on the fifth lens and correct the optical distortion and TV distortion. In addition, the surface of the fifth lens can have better optical path adjustment capability to improve imaging quality.

According to the present invention, an optical imaging system is provided, which includes a first lens, a second lens, a third lens, a fourth lens, a fifth lens, and an imaging plane in order from the object side to the image side. The material of the first lens is glass, and the material of at least one of the second lens to the fifth lens is plastic, and the first transparent At least one lens from the mirror to the fifth lens has a positive refractive power. The focal lengths of the first lens to the fifth lens are f1, f2, f3, f4, and f5. The focal length of the optical imaging system is f. The optical imaging The entrance pupil diameter of the lens system is HEP, the first lens object side to the imaging plane has a distance HOS on the optical axis, and the first lens object side to the fifth lens image side has a distance InTL on the optical axis, The intersection of any surface of any one of these lenses with the optical axis is the starting point, and the contour of the surface is continued until the coordinate point on the surface at a vertical height from the optical axis 1/2 the entrance pupil diameter, the aforementioned two points The length of the profile curve between is ARE, which satisfies the following conditions: 1.0≦f/HEP≦10; 0.5≦HOS/f≦3; and 0.1≦2 (ARE/HEP)≦2.0.

According to the present invention, an optical imaging system is further provided, which includes a first lens, a second lens, a third lens, a fourth lens, a fifth lens, and an imaging surface in order from the object side to the image side. The material of the first lens is glass and the object side and the image side are both flat. The material of at least one of the second lens to the fifth lens is plastic. The focal lengths of the first lens to the fifth lens are f1, f2, f3, f4, and f5, respectively, the focal length of the optical imaging system is f, the diameter of the entrance pupil of the optical imaging lens system is HEP, and the object side of the first lens The imaging surface has a distance HOS on the optical axis, the object side of the first lens to the image side of the fifth lens has a distance InTL on the optical axis, any surface of any of the lenses and the optical axis The intersection point is the starting point, extending the contour of the surface until the coordinate point on the surface at a vertical height of 1/2 the entrance pupil diameter from the optical axis. The length of the contour curve between the two points is ARE, which satisfies the following conditions: 1.0≦ f/HEP≦10; 0.5≦HOS/f≦3; and 0.1≦2 (ARE/HEP)≦2.0.

According to the present invention, an optical imaging system is further provided, which sequentially includes a mechanism light inlet and a first lens from the object side to the image side; the first lens, the second lens, the third lens, the fourth lens, and the fifth lens and One imaging plane. The light inlet of the mechanism restricts the path of light incident on the object side, and has a diameter DDH. The material of a first lens is glass and the object side and the image side are flat. The focal lengths of the first lens to the fifth lens are Are f1, f2, f3, f4, f5, the focal length of the optical imaging system is f, the diameter of the entrance pupil of the optical imaging lens system is HEP, the object side of the first lens to the imaging surface has an optical axis There is a distance HOS, and the distance from the object side of the first lens to the image side of the fifth lens has a distance InTL on the optical axis. The intersection of any surface of any of the lenses and the optical axis is the starting point, which extends along the surface The contour is up to the coordinate point on the surface at a vertical height of 1/2 the entrance pupil diameter from the optical axis. The length of the contour curve between the two points is ARE, which satisfies the following conditions: 1.0≦f/HEP≦10; 0.5≦HOS /f≦3; DDH≦10mm; and 0.1≦2(ARE/HEP)≦2.0.

The length of the contour curve of any surface of a single lens within the maximum effective radius affects the ability of the surface to correct aberrations and optical path differences between light rays of various fields. The longer the length of the contour curve, the better the ability to correct aberrations, but at the same time It will increase the difficulty of manufacturing, so it is necessary to control the length of the contour curve of any surface of a single lens within the maximum effective radius, especially the length of the contour curve (ARS) and the surface within the maximum effective radius of the surface The ratio between the thickness (TP) of the lens on the optical axis (ARS/TP). For example, the length of the contour curve of the maximum effective radius of the first lens object side is represented by ARS11, the thickness of the first lens on the optical axis is TP1, the ratio between the two is ARS11/TP1, and the maximum effective radius of the image side of the first lens The length of the profile curve is represented by ARS12, and the ratio between it and TP1 is ARS12/TP1. The length of the profile curve of the maximum effective radius of the object side of the second lens is represented by ARS21, the thickness of the second lens on the optical axis is TP2, the ratio between the two is ARS21/TP2, and the profile of the maximum effective radius of the image side of the second lens The length of the curve is represented by ARS22, and the ratio between it and TP2 is ARS22/TP2. The proportional relationship between the length of the contour curve of the maximum effective radius of any surface of the remaining lenses in the optical imaging system and the thickness of the lens on the optical axis (TP) to which the surface belongs, and its representation is the same.

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

When |f1|>f5, the total height of the optical imaging system (HOS; Height of Optic) System) can be properly shortened to achieve the purpose of miniaturization.

When |f2|+|f3|+|f4| and |f1|+|f5| satisfy the above conditions, at least one of the second lens to the fourth 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 10. When at least one of the second lens to the fourth lens 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; otherwise, if the second lens to the fourth lens At least one of the four lenses has a weak negative refractive power, and the aberration of the correction system can be fine-tuned.

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

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: object side

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

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

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

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 side

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

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

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

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

152, 252, 352, 452, 552, 652: object side

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

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

190, 290, 390, 490, 590, 690: imaging surface

192, 292, 392, 492, 592, 692: image sensing element

f: focal length of optical imaging system

f1: focal length of the first lens

f2: focal length of the second lens

f3: focal length of the third lens

Focal length of fourth lens: f4

f5: focal length of the fifth lens

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

HAF: half of the maximum angle of view of the optical imaging system

NA1: dispersion coefficient of the first lens

NA2, NA3, NA4, NA5: dispersion coefficient of the second lens to the fifth lens

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

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

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

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

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

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

TP2, TP3, TP4, TP5: the thickness of the second to fifth lenses on the optical axis

ΣTP: the sum of the thickness of all lenses with refractive power

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

IN23: the distance between the second lens and the third lens on the optical axis

IN34: the distance between the third lens and the fourth lens on the optical axis

IN45: the distance between the fourth lens and the fifth lens on the optical axis

InRS51: the horizontal displacement distance from the intersection point of the fifth lens object side on the optical axis to the maximum effective radius position of the fifth lens object side on the optical axis

IF511: the inflection point closest to the optical axis on the side of the fifth lens object

SGI511: the amount of subsidence at this point

HIF511: the vertical distance between the reflex point closest to the optical axis and the optical axis on the side of the fifth lens object

IF521: the inflection point closest to the optical axis on the image side of the fifth lens

SGI521: Subsidence amount at this point

HIF521: the vertical distance between the reflex point closest to the optical axis on the image side of the fifth lens and the optical axis

IF512: the second reflex point close to the optical axis on the object side of the fifth lens

SG1512: the amount of subsidence at this point

HIF512: The vertical distance between the inflection point of the second lens object side near the optical axis and the optical axis

IF522: the second reflex point close to the optical axis on the image side of the fifth lens

SGI522: Subsidence amount at this point

HIF522: the vertical distance between the reflex point of the fifth lens image side near the optical axis and the optical axis

C51: Critical point on the side of the fifth lens object

C52: Critical point on the side of the fifth lens image

SGC51: The horizontal displacement distance between the critical point on the side of the fifth lens object and the optical axis

SGC52: The horizontal displacement distance between the critical point on the image side of the fifth lens and the optical axis

HVT51: The vertical distance between the critical point on the side of the fifth lens object and the optical axis

HVT52: The vertical distance between the critical point on the image side of the fifth lens and the optical axis

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

Dg: diagonal length of the image sensing element

InS: distance from aperture to imaging surface

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

InB: the distance from the image side of the fifth lens to the imaging plane

HOI: The image sensing element effectively senses half of the diagonal length of the area (maximum image height)

TDT: TV Distortion of Optical Imaging System at the Formation of Image

ODT: Optical Distortion of Optical Imaging System at the Formation of Image (Optical Distortion)

201, 301, 401, 501, 601: mechanism entrance hole diameter (DDH)

The above and other features of this creation will be explained in detail by referring to the drawings.

FIG. 1A is a schematic diagram illustrating the optical imaging system of the first embodiment of the present invention; FIG. 1B sequentially illustrates the spherical aberration, astigmatism and optical distortion of the optical imaging system of the first embodiment of the present invention from left to right. Fig. 1C is a diagram showing the meridional plane fan and sagittal plane fan of the optical imaging system of the first embodiment of the optical imaging system of the present invention, the longest operating wavelength and the shortest operating wavelength passing through the edge of the aperture at the 0.7 field of view Aberration diagram; Fig. 2A is a schematic diagram showing the optical imaging system of the second embodiment of the present invention; Fig. 2B shows the spherical aberration and astigmatism of the optical imaging system of the second embodiment of the present invention in order from left to right And the graph of optical distortion; Figure 2C shows the meridional plane fan and sagittal plane fan of the optical imaging system of the second embodiment of the present invention, the longest working wavelength and the shortest working wavelength passing through the edge of the aperture at the 0.7 field of view Aberration diagram; FIG. 3A is a schematic diagram of the optical imaging system of the third embodiment of the present invention; FIG. 3B illustrates the spherical aberration and astigmatism of the optical imaging system of the third embodiment of the present invention in order from left to right And the graph of optical distortion; Figure 3C shows the meridional plane fan and sagittal plane fan of the optical imaging system of the third embodiment of the present invention. The longest operating wavelength and the shortest operating wavelength pass through the aperture edge at 0.7 field of view Aberration diagram; FIG. 4A is a schematic diagram showing the optical imaging system of the fourth embodiment of the present invention; FIG. 4B shows the spherical aberration and astigmatism of the optical imaging system of the fourth embodiment of the present invention in order from left to right And the graph of optical distortion; Figure 4C shows the meridional plane fan and sagittal plane fan of the optical imaging system of the fourth embodiment of the present invention, the longest working wavelength and the shortest working wavelength passing through the edge of the aperture at 0.7 field of view Aberration diagram; FIG. 5A is a schematic diagram showing the optical imaging system of the fifth embodiment of the present invention; FIG. 5B shows the spherical aberration and astigmatism of the optical imaging system of the fifth embodiment of the present invention in order from left to right And the graph of optical distortion; Figure 5C is a lateral aberration diagram of the meridional plane fan and sagittal plane fan of the optical imaging system of the fifth embodiment of the present invention, the longest working wavelength and the shortest working wavelength passing through the edge of the aperture at the 0.7 field of view; Figure 6A It is a schematic diagram showing the optical imaging system of the sixth embodiment of the present invention; FIG. 6B sequentially shows the graphs of spherical aberration, astigmatism and optical distortion of the optical imaging system of the sixth embodiment of the present invention from left to right; FIG. 6C is a lateral aberration diagram of the meridional plane fan and sagittal plane fan of the optical imaging system according to the sixth embodiment of the present invention, with the longest operating wavelength and the shortest operating wavelength passing through the edge of the aperture at 0.7 field of view.

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

The optical imaging system can be designed using three working wavelengths, namely 486.1nm, 587.5nm, and 656.2nm, of which 587.5nm is the main reference wavelength and the main reference wavelength for extracting technical features. The optical imaging system can also be designed using five operating wavelengths, namely 470nm, 510nm, 555nm, 610nm, and 650nm, of which 555nm is the main reference wavelength and the main reference wavelength for extracting 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 lenses with negative refractive power is ΣNPR. It helps to control the total refractive power and total length of the optical imaging system when the following conditions are met: 0.5≦ΣPPR/｜ΣNPR｜≦3.0, preferably Ground, the following conditions can be satisfied: 1≦ΣPPR/|ΣNPR|≦2.5.

The optical imaging system may further include an image sensing element, which is disposed on the imaging surface. The image sensing element effectively senses half the diagonal length of the area (that is, the imaging height or maximum of the optical imaging system (Image height) is HOI, and the distance from the object side of the first lens to the imaging surface on the optical axis is HOS, which satisfies the following conditions: HOS/HOI≦25; and 0.5≦HOS/f≦25. Preferably, the following conditions can be satisfied: 1≦HOS/HOI≦20; and 1≦HOS/f≦20. In this way, the miniaturization of the optical imaging system can be maintained for mounting on thin and light portable electronic products.

In addition, in the optical imaging system of the present invention, at least one aperture can be set according to requirements 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 center aperture, where the front aperture means the aperture is set between the subject and the first lens, and the center aperture means the aperture is set between the first lens and Between imaging planes. If the aperture is the front aperture, the exit pupil of the optical imaging system can form a longer distance from the imaging surface to accommodate more optical elements, and the efficiency of the image sensing element to receive images can be increased; if it is a center aperture, the system It helps to expand the field of view of the system, so that the optical imaging system has the advantages of a wide-angle lens. The distance between the aforementioned aperture and the imaging surface is InS, which satisfies the following condition: 0.2≦InS/HOS≦1.1. With this, it is possible to simultaneously maintain the miniaturization of the optical imaging system and the characteristics of having a wide angle.

In the optical imaging system of this creation, the distance between the object side of the first lens and the image side of the fifth lens is InTL, and the total thickness of all lenses with refractive power on the optical axis is ΣTP, which satisfies the following conditions: 0.1≦ΣTP/ InTL≦0.9. In this way, the contrast of system imaging and the yield of lens manufacturing can be taken into account at the same time, and an appropriate back focal length 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|<100. In this way, the first lens has an appropriate positive refractive power strength to prevent the spherical aberration from increasing too fast. Preferably, the following condition can be satisfied: 0.05<|R1/R2|<80.

The radius of curvature of the object side of the fifth lens is R9, and the radius of curvature of the image side of the fifth lens is R10, which satisfies the following conditions: -50<(R9-R10)/(R9+R10)<50. In this way, it is beneficial to correct the astigmatism generated by the optical imaging system.

The separation distance between the first lens and the second lens on the optical axis is IN12, which satisfies the following Pieces: IN12/f≦5.0. This helps to improve the chromatic aberration of the lens to improve its performance.

The separation distance between the fourth lens and the fifth lens on the optical axis is IN45, which satisfies the following condition: IN45/f≦5.0. This helps to improve the chromatic aberration of the lens to improve its performance.

The thicknesses of the first lens and the second lens on the optical axis are TP1 and TP2, respectively, which satisfy the following conditions: 0.1≦(TP1+IN12)/TP2≦50.0. In this way, it helps to control the sensitivity of optical imaging system manufacturing and improve its performance.

The thicknesses of the fourth lens and the fifth lens on the optical axis are TP4 and TP5, respectively. The separation distance between the two lenses on the optical axis is IN45, which satisfies the following condition: 0.1≦(TP5+IN45)/TP4≦50.0. In this way, it helps to control the sensitivity of optical imaging system manufacturing and reduce the overall height of the system.

The thickness of the second lens, the third lens, and the fourth lens on the optical axis are TP2, TP3, and TP4, respectively. The distance between the second lens and the third lens on the optical axis is IN23, and the distance between the third lens and the fourth lens is The separation distance on the optical axis is IN34, and the distance between the object side of the first lens and the image side of the fifth lens is InTL, which satisfies the following condition: 0.1≦TP3/(IN23+TP3+IN34)<1. In this way, it helps layer by layer to slightly correct the aberration generated by the incident light traveling process and reduce the total height of the system.

In the optical imaging system of this invention, the vertical distance between the critical point C51 of the fifth lens object side and the optical axis is HVT51, the vertical distance between the critical point C52 of the fifth lens image side and the optical axis is HVT52, and the fifth lens object side is The horizontal displacement distance from the intersection point on the optical axis to the critical point C51 at the optical axis is SGC51, and the horizontal displacement distance from the intersection point on the optical axis of the fifth lens image side to the critical point C52 at the optical axis is SGC52, which satisfies the following conditions : 0mm≦HVT51≦3mm; 0mm<HVT52≦6mm; 0≦HVT51/HVT52; 0mm≦|SGC51|≦0.5mm; 0mm<|SGC52|≦2mm; and 0<|SGC52|/(|SGC52|+TP5) ≦0.9. With this, the aberration of the off-axis field of view can be effectively corrected.

The optical imaging system of this creation meets the following conditions: 0.2≦HVT52/HOI≦0.9. Preferably, the following condition can be satisfied: 0.3≦HVT52/HOI≦0.8. This helps optical Aberration correction of the peripheral field of view of the image system.

The optical imaging system of this creation meets the following conditions: 0≦HVT52/HOS≦0.5. Preferably, the following condition can be satisfied: 0.2≦HVT52/HOS≦0.45. This helps to correct the aberration of the peripheral field of view of the optical imaging system.

In the optical imaging system of the present invention, the horizontal displacement distance between the intersection point of the fifth lens object side on the optical axis and the inflection point of the closest optical axis of the fifth lens object side parallel to the optical axis is represented by SGI511, and the fifth lens image The horizontal displacement distance between the intersection point of the side on the optical axis and the reflex point of the closest optical axis of the fifth lens image side parallel to the optical axis is represented by SGI521, which satisfies the following conditions: 0<SGI511/(SGI511+TP5)≦0.9 ; 0<SGI521/(SGI521+TP5)≦0.9. Preferably, the following conditions can be satisfied: 0.1≦SGI511/(SGI511+TP5)≦0.6; 0.1≦SGI521/(SGI521+TP5)≦0.6.

The horizontal displacement distance between the intersection point of the fifth lens object side on the optical axis and the reflex point of the second lens object side near the optical axis parallel to the optical axis is expressed by SGI512. The image side of the fifth lens on the optical axis The horizontal displacement distance between the intersection point and the reflex point near the optical axis of the fifth lens image side parallel to the optical axis is expressed by SGI522, which satisfies the following conditions: 0<SGI512/(SGI512+TP5)≦0.9; 0<SGI522 /(SGI522+TP5)≦0.9. Preferably, the following conditions can be satisfied: 0.1≦SGI512/(SGI512+TP5)≦0.6; 0.1≦SGI522/(SGI522+TP5)≦0.6.

The vertical distance between the reflex point of the closest optical axis of the fifth lens object side and the optical axis is represented by HIF511, the intersection point of the fifth lens image side on the optical axis to the reflex point and optical axis of the closest optical axis of the fifth lens image side The vertical distance between them is expressed by HIF521, which satisfies the following conditions: 0.001mm≦|HIF511|≦5mm; 0.001mm≦|HIF521|≦5mm. Preferably, the following conditions can be satisfied: 0.1mm≦|HIF511|≦3.5mm; 1.5mm≦|HIF521|≦3.5mm.

The vertical distance between the second reflex point near the optical axis of the fifth lens object side and the optical axis is expressed by HIF512, and the intersection point of the fifth lens image side on the optical axis to the second lens side reflex of the fifth lens image side The vertical distance between the point and the optical axis is expressed by HIF522, which meets the following conditions: 0.001mm≦ ｜HIF512｜≦5mm; 0.001mm≦|HIF522|≦5mm. Preferably, the following conditions can be satisfied: 0.1mm≦|HIF522|≦3.5mm; 0.1mm≦|HIF512|≦3.5mm.

The vertical distance between the third reflex point near the optical axis of the fifth lens object side and the optical axis is represented by HIF513, and the intersection point of the fifth lens image side on the optical axis to the third near optical axis recurve of the fifth lens image side The vertical distance between the point and the optical axis is represented by HIF523, which satisfies the following conditions: 0.001mm≦|HIF513|≦5mm; 0.001mm≦|HIF523|≦5mm. Preferably, the following conditions can be satisfied: 0.1mm≦|HIF523|≦3.5mm; 0.1mm≦|HIF513|≦3.5mm.

The vertical distance between the fourth inflection point of the fifth lens object side near the optical axis and the optical axis is represented by HIF514, and the intersection of the fifth lens image side on the optical axis to the fourth lens side image inversion of the fifth lens side The vertical distance between the point and the optical axis is represented by HIF524, which satisfies the following conditions: 0.001mm≦|HIF514|≦5mm; 0.001mm≦|HIF524|≦5mm. Preferably, the following conditions can be satisfied: 0.1mm≦|HIF524|≦3.5mm; 0.1mm≦|HIF514|≦3.5mm.

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

The equation system of the above aspheric surface is: z=ch2/[1+[1(k+1)c2h2]0.5]+A4h4+A6h6+A8h8+A10h10+A12h12+A14h14+A16h16+A18h18+A20h20+... (1)

Where z is the position value along the optical axis at the height h with the surface vertex as a reference, k is the cone coefficient, 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 lens can be made of plastic or glass. When the lens material is plastic, it can effectively reduce the production cost and weight. In addition, when the material of the lens is glass, the thermal effect can be controlled and the design space for the configuration of the refractive power of the optical imaging system can be increased. In addition, the object side and the image side of the first lens to the fifth lens in the optical imaging system can be aspherical, which can obtain more In addition to reducing aberrations, the use of control variables can even reduce the number of lenses used compared to traditional glass lenses, thus effectively reducing the total height of the original optical imaging system.

Furthermore, in the optical imaging system provided by this work, if the lens surface is convex, in principle, the lens surface is convex at the low optical axis; if the lens surface is concave, in principle, the lens surface is at the low optical axis. Concave.

The optical imaging system of this creation can be applied to the mobile focusing optical system according to the visual demand, and has the characteristics of excellent aberration correction and good imaging quality, thereby expanding the application level.

The more visible requirements of the optical imaging system of the present invention include a driving module, which 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-shake element (OIS) for reducing the frequency of out-of-focus caused by lens vibration during the shooting process.

The optical imaging system of the present invention can make the first lens, the second lens, the third lens, the fourth lens, and the fifth lens at least one lens a light filtering element with a wavelength less than 500 nm according to the demand, which can be determined by the specific tool The coating on at least one surface of the lens with the filtering function or the lens itself is made of a material with a filterable short wavelength.

The imaging surface of the created optical imaging system can be selected as a flat surface or a curved surface according to the needs. When the imaging surface is a curved surface (such as a spherical surface with a radius of curvature), it helps to reduce the incident angle required to focus light on the imaging surface. In addition to helping to achieve the length of the miniature optical imaging system (TTL), Illumination also helps.

The electronic device loaded with the optical imaging system created by this invention may have a mechanism light entrance hole on the object side. Please refer to FIG. 7, the aforementioned mechanism light entrance hole may be the front lens opening of the electronic device, which may To limit the path of light incident on the object side, the diameter of the light inlet of the mechanism is expressed in DDH. The optical imaging system of the present invention may include at least one reflective element, such as prisms or reflective mirrors, which can improve the spatial distribution and application of the imaging system at the terminal, and allow the imaging system to be used in limited Increase the total number of lenses in the construction space. The aforementioned reflective element may be disposed between the lenses in the optical imaging system, which is beneficial to reduce the aperture of the mechanism before the light enters the first lens. In addition, the reflective element can also be disposed on the object side end of the first lens, which is beneficial to shorten the total system length of the optical imaging system. The number of reflecting elements can be more than two according to the requirements, and the setting method of the reflecting surface can be adjusted according to the requirements such as space configuration. According to the requirements, the materials with suitable refractive index or dispersion coefficient, such as glass or plastic, can be used. The thickness of 稜鏡 (referred to the total length of the path of the internal optical axis of 稜鏡) is expressed by PT, which is mainly composed of the ray path PT1 of the incident section (that is, the central field of view or the optical axis) and the ray path PT2 of the exit section (that is, the central field of view Light or optical axis), that is, PT=PT1+PT2. The thickness of 稜鏡 is mainly affected by the refractive index of its material, the angle of view of the optical imaging system and the size of the aperture.

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

First embodiment

Please refer to FIGS. 1A and 1B, in which FIG. 1A shows a schematic diagram of an optical imaging system according to the first embodiment of the present creation, and FIG. 1B is from left to right in order for the optical imaging system of the first embodiment. Graph of spherical aberration, astigmatism and optical distortion. FIG. 1C is a lateral aberration diagram of the meridional plane fan and the sagittal plane fan of the optical imaging system of the first embodiment, with the longest operating wavelength and the shortest operating wavelength passing through the aperture edge at the 0.7 field of view. FIG. 1D is a numerical diagram showing the relative illuminance of each field of view of the optical imaging system of the optical imaging system of the first embodiment of the present invention on the imaging plane. As can be seen from FIG. 1A, the optical imaging system includes a first lens 110, an aperture 100, a second lens 120, a third lens 130, a fourth lens 140, a fifth lens 150, and an infrared filter in order from the object side to the image side 180, the imaging surface 190 and the image sensing element 192.

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

The horizontal displacement distance between the intersection of the first lens object side on the optical axis and the reflex point of the closest optical axis of the first lens side parallel to the optical axis is represented by SGI111, and the reflex point of the closest optical axis of the first lens image side The horizontal displacement distance between the parallel to the optical axis is represented by SGI121, which satisfies the following conditions: SGI111=1.96546mm; |SGI111|/(|SGI111|+TP1)=0.72369.

The vertical distance between the reflex point of the closest optical axis of the object side of the first lens and the optical axis is represented by HIF111, and the vertical distance between the reflex point of the closest optical axis of the image side of the first lens and the optical axis is represented by HIF121, which satisfies the following conditions : HIF111=3.38542mm; HIF111/HOI=0.90519.

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

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

The vertical distance between the reflex point of the closest optical axis of the object side of the second lens and the optical axis is represented by HIF211, and the vertical distance between the reflex point of the closest optical axis of the image side of the second lens and the optical axis is represented by HIF221.

The third lens 130 has a positive refractive power and is made of plastic material. Its object side 132 is convex, its image side 134 is convex, and both are aspherical, and its object side 132 has an inflection point. The length of the profile curve of the maximum effective radius of the object side of the third lens is represented by ARS31, the maximum of the image side of the third lens The effective radius of the contour curve length is represented by ARS32. The profile curve length of the 1/2 entrance pupil diameter (HEP) on the object side of the third lens is represented by ARE31, and the profile curve length of the 1/2 entrance pupil diameter (HEP) on the image side of the third lens is represented by ARE32. The thickness of the third lens on the optical axis is TP3.

The horizontal displacement distance between the intersection point of the third lens object side on the optical axis and the reflex point of the closest optical axis of the third lens object side parallel to the optical axis is represented by SGI311, and the intersection point of the third lens image side on the optical axis to The horizontal displacement distance between the reflex points of the closest optical axis of the third lens image side and the optical axis is represented by SGI321, which satisfies the following conditions: SGI311=0.00388mm; |SGI311|/(|SGI311|+TP3)=0.00414.

The horizontal displacement distance between the intersection point of the third lens object side on the optical axis and the second lens object side's inflection point near the optical axis parallel to the optical axis is represented by SGI312, and the third lens image side on the optical axis The horizontal displacement distance parallel to the optical axis between the intersection point and the second lens-side reflex point near the optical axis of the third lens image is represented by SGI322.

The vertical distance between the reflex point of the closest optical axis of the third lens object side and the optical axis is represented by HIF311, and the vertical distance between the reflex point of the closest optical axis of the third lens image side and the optical axis is represented by HIF321, which satisfies the following conditions : HIF311=0.38898mm; HIF311/HOI=0.10400.

The vertical distance between the second reflex point near the optical axis of the third lens object side and the optical axis is represented by HIF412, and the vertical distance between the second reflex point near the optical axis of the fourth lens image side and the optical axis is represented by HIF422.

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

The horizontal displacement distance between the intersection point of the fourth lens object side on the optical axis and the reflex point of the closest optical axis of the fourth lens object side parallel to the optical axis is represented by SGI411, and the intersection point of the fourth lens image side on the optical axis to The horizontal displacement distance between the reflex points of the closest optical axis of the fourth lens image side and the optical axis is represented by SGI421, which satisfies the following conditions: SGI421=0.06508mm; |SGI421|/(|SGI421|+TP4)=0.03459.

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

The vertical distance between the reflex point of the closest optical axis of the fourth lens object side and the optical axis is represented by HIF411, and the vertical distance between the reflex point of the closest optical axis of the fourth lens image side and the optical axis is represented by HIF421, which satisfies the following conditions : HIF421=0.85606mm; HIF421/HOI=0.22889.

The vertical distance between the second reflex point near the optical axis of the fourth lens object side and the optical axis is represented by HIF412, and the vertical distance between the second reflex point near the optical axis of the fourth lens image side and the optical axis is represented by HIF422.

The fifth lens 150 has negative refractive power and is made of plastic material. Its object side 152 is concave, its image side 154 is concave, and both are aspherical, and its object side 152 and image side 154 both have an inflection point. The profile curve length of the maximum effective radius of the fifth lens object side is represented by ARS51, and the profile curve length of the maximum effective radius of the fifth lens image side is represented by ARS52. The profile curve length of the 1/2 entrance pupil diameter (HEP) on the object side of the fifth lens is represented by ARE51, and the profile curve length of the 1/2 entrance pupil diameter (HEP) on the image side of the fifth lens is represented by ARE52. The thickness of the fifth lens on the optical axis is TP5.

The horizontal displacement distance between the intersection of the fifth lens object side on the optical axis and the reflex point of the closest optical axis of the fifth lens object side parallel to the optical axis is represented by SGI511, and the intersection point of the fifth lens image side on the optical axis to The horizontal displacement distance between the reflex point of the closest optical axis of the side of the fifth lens image parallel to the optical axis is SGI521 indicates that it satisfies the following conditions: SGI511=-1.51505mm; |SGI511|/(|SGI511|+TP5)=0.70144; SGI521=0.01229mm;|SGI521|/(|SGI521|+TP5)=0.01870.

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

The vertical distance between the reflex point of the closest optical axis of the fifth lens object side and the optical axis is represented by HIF511, and the vertical distance between the reflex point of the closest optical axis of the fifth lens image side and the optical axis is represented by HIF521, which satisfies the following conditions : HIF511=2.25435mm; HIF511/HOI=0.60277; HIF521=0.82313mm; HIF521/HOI=0.22009.

The vertical distance between the second reflex point near the optical axis of the fifth lens object side and the optical axis is represented by HIF512, and the vertical distance between the second reflex point near the optical axis of the fifth lens image side and the optical axis is represented by HIF522.

The infrared filter 180 is made of glass, which is disposed between the fifth lens 150 and the imaging surface 190 and does not affect the focal length of the optical imaging system.

In the optical imaging system of this embodiment, the focal length of the optical imaging system is f, the diameter of the entrance pupil of the optical imaging system is HEP, and the half of the maximum angle of view in the optical imaging system is HAF. The values are as follows: f=3.03968mm; f/HEP =1.6; and HAF=50.001 degrees and tan(HAF)=1.1918.

In the optical imaging system of this embodiment, the focal length of the first lens 110 is f1, and the focal length of the fifth lens 150 is f5, which satisfies the following conditions: f1=-9.24529mm; |f/f1|=0.32878; f5=-2.32439 ; And |f1|>f5.

In the optical imaging system of this embodiment, the focal lengths of the second lens 120 to the fifth lens 150 are f2, f3, f4, and f5, respectively, which satisfy the following conditions: |f2|+|f3|+|f4|=17.3009mm; ｜f1｜+ |f5|=11.5697mm and |f2|+|f3|+|f4|>|f1|+|f5|

The ratio PPR of the focal length f of the optical imaging system to the focal length fp of each lens with positive refractive power, the ratio NPR of the focal length f of the optical imaging system to the focal length fn of each lens with negative refractive power, optical imaging in this embodiment In the system, the total PPR of all lenses with positive refractive power is ΣPPR=f/f2+f/f3+f/f4=1.86768, and the total NPR of all lenses with negative refractive power is ΣNPR=f/f1+f/f5=- 1.63651, ΣPPR/|ΣNPR|=1.14125. At the same time, the following conditions are also satisfied: |f/f2|=0.47958;|f/f3|=0.38289;|f/f4|=1.00521;|f/f5|=1.30773.

In the optical imaging system of this embodiment, the distance between the first lens object side 112 to the fifth lens image side 154 is InTL, the distance between the first lens object side 112 to the imaging plane 190 is HOS, and the aperture 100 to the imaging plane 180 The distance between them is InS, the half of the diagonal length of the effective sensing area of the image sensing element 192 is HOI, and the distance between the image side 154 of the fifth lens and the imaging surface 190 is BFL, which satisfies the following conditions: InTL+BFL=HOS ; HOS=10.56320mm; HOI=3.7400mm; HOS/HOI=2.8244; HOS/f=3.4751; InS=6.21073mm; and InS/HOS=0.5880.

In the optical imaging system of this embodiment, the total thickness of all lenses with refractive power on the optical axis is ΣTP, which satisfies the following conditions: ΣTP=5.0393mm; InTL=9.8514mm and ΣTP/InTL=0.5115. In this way, the contrast of system imaging and the yield of lens manufacturing can be taken into account at the same time, and an appropriate back focal length can be provided to accommodate other components.

In the optical imaging system of this embodiment, the radius of curvature of the object side 112 of the first lens is R1, and the radius of curvature of the image side 114 of the first lens is R2, which satisfies the following conditions: |R1/R2|=1.9672. In this way, the first lens has an appropriate positive refractive power strength to prevent the spherical aberration from increasing too fast.

In the optical imaging system of this embodiment, the curvature radius of the fifth lens object side 152 is R9, and the curvature radius of the fifth lens image side 154 is R10, which satisfies the following conditions: (R9-R10)/(R9+R10)= -1.1505. In this way, it is beneficial to correct the astigmatism generated by the optical imaging system.

In the optical imaging system of this embodiment, the total focal length of all lenses with positive refractive power For ΣPP, it satisfies the following conditions: ΣPP=f2+f3+f4=17.30090mm; and f2/(f2+f3+f4)=0.36635. In this way, it is helpful to appropriately distribute the positive refractive power of the second lens 120 to other positive lenses, so as to suppress the generation of significant aberrations in the process of the incident light.

In the optical imaging system of this embodiment, the total focal length of all lenses with negative refractive power is ΣNP, which satisfies the following conditions: ΣNP=f1+f5=-11.56968mm; and f5/(f1+f5)=0.20090. In this way, it is helpful to appropriately distribute the negative refractive power of the fifth lens to other negative lenses, so as to suppress the generation of significant aberrations in the process of the incident light.

In the optical imaging system of this 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: 1N12=3.19016mm; IN12/f=1.04951. This helps to improve the chromatic aberration of the lens to improve its performance.

In the optical imaging system of this embodiment, the separation distance between the fourth lens 140 and the fifth lens 150 on the optical axis is IN45, which satisfies the following conditions: 1N45=0.40470mm; IN45/f=0.13314. This helps to improve the chromatic aberration of the lens to improve its performance.

In the optical imaging system of this embodiment, the thicknesses of the first lens 110, the second lens 120, and the third lens 130 on the optical axis are TP1, TP2, and TP3, respectively, which satisfy the following conditions: TP1=0.75043mm; TP2=0.89543 mm; TP3=0.93225mm; and (TP1+IN12)/TP2=4.40078. In this way, it helps to control the sensitivity of optical imaging system manufacturing and improve its performance.

In the optical imaging system of this embodiment, the thicknesses of the fourth lens 140 and the fifth lens 150 on the optical axis are TP4 and TP5, respectively. The separation distance between the two lenses on the optical axis is IN45, which satisfies the following conditions: TP4= 1.81634mm; TP5=0.64488mm; and (TP5+IN45)/TP4=0.57785. In this way, it helps to control the sensitivity of optical imaging system manufacturing and reduce the overall height of the system.

In the optical imaging system of this embodiment, the distance between the third lens 130 and the fourth lens 140 on the optical axis is IN34, and the distance between the first lens object side 112 and the fifth lens image side 164 is InTL, which satisfies the following Conditions: TP2/TP3=0.96051; TP3/TP4=0.51325; TP4/TP5= 2.81657; and TP3/(IN23+TP3+IN34)=0.43372. This helps to slightly correct the aberrations caused by the incident light traveling and reduce the total height of the system.

In the optical imaging system of this embodiment, the horizontal displacement distance from the intersection point of the fourth lens object side 142 on the optical axis to the maximum effective radius position of the fourth lens object side 142 on the optical axis is InRS41, and the fourth lens image side 144 is The horizontal displacement distance from the intersection point on the optical axis to the maximum effective radius position of the fifth lens image side 144 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=-0.09737mm ; InRS42=-1.31040mm; | InRS41|/TP4=0.05361 and |InRS42|/TP4=0.72145. In this way, it is conducive to 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 of the fourth lens object side 142 and the optical axis is HVT41, and the vertical distance between the critical point of the fourth lens image side 144 and the optical axis is HVT42, which satisfies the following conditions: HVT41=1.41740mm; HVT42=0

In the optical imaging system of this embodiment, the horizontal displacement distance from the intersection of the fifth lens object side 152 on the optical axis to the maximum effective radius position of the fifth lens object side 152 on the optical axis is InRS51, and the fifth lens image side 154 is The horizontal displacement distance from the intersection point on the optical axis to the maximum effective radius of the fifth lens image side 154 on the optical axis is InRS52, and the thickness of the fifth lens 150 on the optical axis is TP5, which satisfies the following conditions: InRS51=-1.63543mm ; InRS52=-0.34495mm; | InRS51|/TP5=2.53604 and |InRS52|/TP5=0.53491. In this way, it is conducive to 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 of the fifth lens object side 162 and the optical axis is HVT51, and the vertical distance between the critical point of the fifth lens image side 154 and the optical axis is HVT52, which satisfies the following conditions: HVT51=0; HVT52=1.35891mm; and HVT51/HVT52=0.

In the optical imaging system of this embodiment, it satisfies the following conditions: HVT52/HOI= 0.36334. This helps to correct the aberration of the peripheral field of view of the optical imaging system.

In the optical imaging system of this embodiment, it satisfies the following condition: HVT52/HOS=0.12865. This helps to correct the aberration of the peripheral field of view of the optical imaging system.

In the optical imaging system of this embodiment, the third lens and the fifth lens have negative refractive power, the third lens has a dispersion coefficient of NA3, and the fifth lens has a dispersion coefficient of NA5, which satisfies the following condition: NA5/NA3=0.368966. This helps to correct the chromatic aberration of the optical imaging system.

In the optical imaging system of this embodiment, the TV distortion of the optical imaging system during image formation becomes TDT, and the optical distortion during image formation becomes ODT, which satisfies the following conditions: |TDT|=0.63350%;|ODT|=2.06135%.

In the optical imaging system of this embodiment, the longest operating wavelength of the positive meridian plane fan pattern is incident on the imaging plane through the aperture edge. The lateral aberration of 0.7 field of view is expressed by PLTA, which is -0.042mm, the positive meridian plane light The shortest operating wavelength of the fan image is incident on the imaging plane through the aperture edge. The lateral aberration of the field of view is expressed as PSTA, which is 0.056mm. The longest operating wavelength of the negative meridian light fan image is incident on the imaging surface through the aperture edge. 0.7 The lateral aberration of the field of view is expressed in NLTA, which is -0.011mm, the shortest working wavelength of the negative meridian plane fan pattern is incident on the imaging plane through the aperture edge. The lateral aberration of the 0.7 field of view is expressed in NSTA, which is -0.024 mm. The longest operating wavelength of the sagittal plane fan pattern is incident on the imaging plane through the aperture edge. The lateral aberration of the 0.7 field of view is expressed in SLTA, which is -0.013mm, and the shortest operating wavelength of the sagittal plane fan diagram is incident on the imaging plane through the aperture edge. The lateral aberration of the upper 0.7 field of view is represented by SSTA, which is 0.018mm.

Refer to Table 1 and Table 2 below.

Table 2. Aspheric coefficients of the first embodiment

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

Table 1 is the detailed structural data of the first embodiment of FIG. 1, in which the units of radius of curvature, thickness, distance and focal length are mm, and surfaces 0-16 sequentially represent the surface from the object side to the image side. Table 2 is the aspherical data in the first embodiment, where k is the conical coefficient in the aspherical curve equation, and A1-A20 represents the aspherical coefficients of the 1st to 20th orders of each surface. In addition, the following tables of the embodiments correspond to the schematic diagrams and aberration curve diagrams of the embodiments. The definitions of the data in the tables are the same as the definitions of Table 1 and Table 2 of the first embodiment, and are not repeated here.

Second embodiment

Please refer to FIG. 2A and FIG. 2B, wherein FIG. 2A shows a schematic diagram of an optical imaging system according to the second embodiment of the present creation, and FIG. 2B is from left to right in order for the optical imaging system of the second embodiment. Graph of spherical aberration, astigmatism and optical distortion. FIG. 2C is a lateral aberration diagram of the optical imaging system of the second embodiment at a field of view of 0.7. As can be seen from FIG. 2A, the optical imaging system includes, from the object side to the image side, a first lens 210, an aperture 200, a second lens 220, a third lens 230, a fourth lens 240, a fifth lens 250, and an infrared filter 280, the imaging surface 290, and the image sensing element 292.

The electronic device loaded in this embodiment may have a mechanism light entrance hole 201 on the object side, which restricts the path of light incident on the object side. The mechanism light entrance hole 201 has a diameter DDH=1.967 mm. The light entrance hole 201 of the mechanism is 0.2 mm away from the objective side lens center (where the optical axis passes) of the first lens 210.

The first lens 210 has a positive refractive power and is made of glass. Its object side 212 is flat, its image side 214 is flat, and it is flat glass, and its focal length is infinity (INF).

The second lens 220 has a positive refractive power and is made of plastic material. Its object side 222 is convex, its image side 224 is convex, and both are aspherical, and its object side 222 has two inflexions and an image side 224 has an inflection point.

The third lens 230 has a negative refractive power and is made of plastic material. Its object side 232 is concave, its image side 234 is concave, and both are aspherical, and its object side 232 has a tri-reflection point and the image side 234 has a Recurve point.

The fourth lens 240 has positive refractive power and is made of plastic material. Its object side 242 is concave, its image side 244 is convex, and both are aspherical, and its object side 242 has two inflexions and the image side 244 has a Recurve point.

The fifth lens 250 has a negative refractive power and is made of plastic material. Its object side 252 is convex, its image side 254 is concave, and both are aspherical, and its object side 242 has two inflexions and the image side 244 has a Recurve point. In this way, the angle of incidence of the off-axis field of view light can be effectively suppressed, and the aberration of the off-axis field of view can be further corrected.

The infrared filter 280 is made of glass, which is disposed between the fifth lens 250 and the imaging surface 290 and does not affect the focal length of the optical imaging system.

Please refer to Table 3 and Table 4 below.

In the second embodiment, the curve equation of the aspherical 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.

The following conditional values can be obtained according to Table 3 and Table 4:

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

The following values can be obtained according to Table 3 and Table 4:

Third embodiment

Please refer to FIG. 3A and FIG. 3B, wherein FIG. 3A shows a schematic diagram of an optical imaging system according to the third embodiment of the present creation, and FIG. 3B is from left to right in order for the optical imaging system of the third embodiment. Graph of spherical aberration, astigmatism and optical distortion. FIG. 3C is a lateral aberration diagram of the optical imaging system of the third embodiment at a field of view of 0.7. As can be seen from FIG. 3A, the optical imaging system includes a first lens 310, an aperture 300, a second lens 320, a third lens 330, a fourth lens 340, a fifth lens 350, and an infrared filter in order from the object side to the image side 380, imaging surface 390, and image sensing element 392.

In the electronic device loaded in this embodiment, there may be a mechanism light entrance hole 301 on the object side, which restricts the path of light incident on the object side. The mechanism light entrance hole 301 has a diameter DDH=1.962 mm. The light entrance hole 301 of the mechanism is 0.2 mm away from the objective side lens center (where the optical axis passes) of the first lens 310.

The first lens 310 has a positive refractive power and is made of glass. Its object side 312 is flat, its image side 314 is flat, and it is flat glass, and its focal length is infinity (INF)

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

The third lens 330 has negative refractive power and is made of plastic material. Its object side 332 is convex, its image side 334 is concave, and both are aspherical, and its object side 332 has two inflexions and the image side 334 has three Recurve point.

The fourth lens 340 has a positive refractive power and is made of plastic material. Its object side 342 is concave, its image side 344 is convex, and both are aspherical, and its object side 342 has two inflexions and the image side 344 has a Recurve point.

The fifth lens 350 has negative refractive power and is made of plastic material. Its object side 352 is convex, its image side 354 is concave, and both are aspherical, and its object side 352 has two inflexions and the image side 354 has a Recurve point. In this way, it is beneficial to shorten the back focal length to maintain miniaturization.

The infrared filter 380 is made of glass, which is disposed between the fifth lens 350 and the imaging surface 390 and does not affect the focal length of the optical imaging system.

Please refer to Table 5 and Table 6 below.

In the third embodiment, the curve equation of the aspherical 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.

The following conditional values can be obtained according to Table 5 and Table 6:

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

The following conditional values can be obtained according to Table 5 and Table 6:

Fourth embodiment

Please refer to FIGS. 4A and 4B, in which FIG. 4A shows a schematic diagram of an optical imaging system according to the fourth embodiment of the present creation, and FIG. 4B is from left to right in order for the optical imaging system of the fourth embodiment. Graph of spherical aberration, astigmatism and optical distortion. FIG. 4C is a lateral aberration diagram of the optical imaging system of the fourth embodiment at a field of view of 0.7. As can be seen from FIG. 4A, the optical imaging system includes a first lens 410, an aperture 400, a second lens 420, a third lens 430, a fourth lens 440, a fifth lens 450, and an infrared filter in order from the object side to the image side 480, imaging surface 490, and image sensing element 492.

In the electronic device loaded in this embodiment, there may be a mechanism light entrance hole 401 on the object side, which restricts the path of light incident on the object side. The mechanism light entrance hole 401 has a diameter DDH=1.950 mm. The light entrance hole 401 of the mechanism is 0.2 mm from the objective side lens center (where the optical axis passes) of the first lens 410.

The first lens 410 has a negative refractive power and is made of glass. Its object side 412 is concave, and its image side 414 is convex, all of which are spherical.

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

The third lens 430 has a negative refractive power and is made of plastic. The object side 432 is convex, the image side 434 is concave, and both are aspherical, and both the object side 432 and the image side 434 have an inflection point.

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

The fifth lens 450 has a negative refractive power and is made of plastic material. Its object side 452 is convex, its image side 454 is concave, and both are aspherical, and its object side 452 has two inflexions and the image side 454 has a Recurve point. In this way, it is beneficial to shorten the back focal length to maintain miniaturization.

The infrared filter 480 is made of glass, which is disposed between the fifth lens 450 and the imaging surface 490 and does not affect the focal length of the optical imaging system.

Please refer to Table 7 and Table 8 below.

In the fourth embodiment, the curve equation of the aspherical surface is expressed as 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.

The following conditional values can be obtained according to Table 7 and Table 8:

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

The following conditional values can be obtained according to Table 7 and Table 8:

Fifth embodiment

Please refer to FIGS. 5A and 5B, wherein FIG. 5A shows a schematic diagram of an optical imaging system according to the fifth embodiment of the present invention, and FIG. 5B is the optical imaging system of the fifth embodiment in order from left to right. Graph of spherical aberration, astigmatism and optical distortion. FIG. 5C is a lateral aberration diagram of the optical imaging system of the fifth embodiment at a field of view of 0.7. As can be seen from FIG. 5A, the optical imaging system includes a first lens 510, an aperture 500, a second lens 520, a third lens 530, a fourth lens 540, a fifth lens 550, and an infrared filter in order from the object side to the image side 580, imaging surface 590, and image sensing element 592.

In the electronic device loaded in this embodiment, there may be a mechanism light entrance hole 501 on the object side, which restricts the path of light incident on the object side. The mechanism light entrance hole 501 has a diameter DDH=1.978 mm. The light entrance hole 501 of the mechanism is 0.2 mm from the objective side lens center (where the optical axis passes) of the first lens 510.

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

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

The third lens 530 has a negative refractive power and is made of plastic material. Its object side 532 is concave, its image side 534 is concave, and both are aspherical, and its object side 532 has four inflexions and the image side 534 has a Recurve point.

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

The fifth lens 550 has a negative refractive power and is made of plastic. Its object side 552 is convex, its image side 554 is concave, and both are aspherical, and its object side 552 has four inverse curvature points and the image side 554 has a Recurve point. In this way, it is beneficial to shorten the back focal length to maintain miniaturization.

The infrared filter 580 is made of glass, which is disposed between the fifth lens 550 and the imaging surface 590 and does not affect the focal length of the optical imaging system.

Please refer to Table 9 and Table 10 below.

In the fifth embodiment, the curve equation of the aspherical 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.

The following conditional values can be obtained according to Table 9 and Table 10:

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

The following conditional values can be obtained according to Table 9 and Table 10:

Sixth embodiment

Please refer to FIGS. 6A and 6B, in which FIG. 6A shows a schematic diagram of an optical imaging system according to the sixth embodiment of the present creation, and FIG. 6B is from left to right in order for the optical imaging system of the sixth embodiment. Graph of spherical aberration, astigmatism and optical distortion. FIG. 6C is a lateral aberration diagram of the optical imaging system of the sixth embodiment at a field of view of 0.7. As can be seen from FIG. 6A, the optical imaging system includes a first lens 610, an aperture 600, a second lens 620, a third lens 630, a fourth lens 640, a fifth lens 650, and an infrared filter in order from the object side to the image side 680, imaging surface 690, and image sensing element 692.

In the electronic device loaded in this embodiment, there may be a mechanism light entrance hole 601 on the object side, which restricts the path of light incident on the object side. The mechanism light entrance hole 601 has a diameter DDH=1.990 mm. The light entrance hole 601 of the mechanism is 0.2 mm from the objective side center of the first lens 610 (where the optical axis passes).

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

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

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

The fourth lens 640 has positive refractive power and is made of plastic material. Its object side 642 is concave, its image side 644 is convex, and both are aspherical, and its image side 644 has an inflexion point.

The fifth lens 650 has a negative refractive power and is made of plastic material. Its object side 652 is convex, its image side 654 is concave, and both are aspherical, and its object side 652 has two inverse curvature points and the image side 654 has a Recurve point. In this way, it is beneficial to shorten the back focal length to maintain miniaturization. In addition, it can also effectively suppress the angle of incidence of the off-axis field of view, and can further correct the aberration of the off-axis field of view.

The infrared filter 680 is made of glass, which is disposed on the fifth lens 650 and the imaging surface 690 It does not affect the focal length of the optical imaging system.

Please refer to Table 11 and Table 12 below.

In the sixth embodiment, the curve equation of the aspherical surface is expressed as 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.

The following conditional values can be obtained according to Table 11 and Table 12:

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

The following conditional values can be obtained according to Table 11 and Table 12:

Although this creation has been disclosed as above by way of implementation, it is not intended to limit this creation. Anyone who is familiar with this skill can make various changes and modifications within the spirit and scope of this creation, so the protection of this creation is protected The scope shall be determined by the scope of the attached patent application.

200: aperture

201: Inlet diameter of mechanism (DDH)

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

250: fifth lens

252: Object side

254: like side

280: imaging surface

290: Infrared filter

292: Image sensor

Claims (25)

An optical imaging system includes, in order from the object side to the image side, a first lens with refractive power; a second lens with refractive power; a third lens with refractive power; a fourth lens with refractive power A fifth lens with refractive power; and an imaging surface, wherein the optical imaging system has five lenses with refractive power, at least one of the first lens to the fifth lens has a positive refractive power, the first The material of the lens is glass, the material of at least one of the second lens to the fifth lens is plastic, and the focal lengths of the first lens to the fifth lens are f1, f2, f3, f4, and f5, respectively. The focal length of the system is f, the entrance pupil diameter of the optical imaging lens system is HEP, the first lens object side to the imaging plane has a distance HOS on the optical axis, and the first lens object side to the fifth lens image side There is a distance InTL on the optical axis, the intersection of any surface of any of these lenses with the optical axis is the starting point, and the contour of the surface is continued until the vertical height of 1/2 the diameter of the entrance pupil on the surface from the optical axis Up to the coordinate point at, the contour curve length between the two points is ARE, which satisfies the following conditions: 1.0≦f/HEP≦2.8; 0.5≦HOS/f≦3.5; and 0.1≦2(ARE/HEP)≦2.0. The optical imaging system according to claim 1, wherein half of the maximum viewing angle of the optical imaging lens system is HAF, which satisfies the following formula: 0deg<HAF≦50deg. The optical imaging system according to claim 1, wherein the second transparent The material from the mirror to the fifth lens is plastic. The optical imaging system according to claim 1, wherein the refractive index of the first lens is Nd1, which satisfies the following formula: 1.70≦Nd1≦3.0. The optical imaging system according to claim 1, wherein the thickness of the first lens is TP1, which satisfies the following formula: 0.5mm≦TP1≦0.9mm. The optical imaging system according to claim 1, wherein the maximum effective radius of any surface of any one of the lenses is represented by EHD, and the intersection point of any surface of any of the lenses and the optical axis is the starting point, The contour of the surface is continued until the maximum effective radius of the surface is the end point. The length of the contour curve between the two points is ARS, which satisfies the following formula: 0.9≦ARS/EHD≦2.0. The optical imaging system according to claim 1, wherein the TV distortion of the optical imaging system at the time of image formation is TDT, the optical imaging system has a maximum imaging height HOI perpendicular to the optical axis on the imaging plane, the optical imaging system The longest operating wavelength of the positive meridian plane fan passes the edge of the entrance pupil and is incident on the imaging plane at 0.7HOI. The lateral aberration is expressed as PLTA, and the shortest operating wavelength of the positive meridian plane fan passes the entrance pupil edge The lateral aberration incident on the imaging plane at 0.7 HOI is represented by PSTA, and the longest operating wavelength of the negative meridian plane fan passes through the entrance pupil edge and is incident on the imaging plane. The lateral aberration incident on the imaging plane at 0.7 HOI is represented by NLTA , The shortest working wavelength of the negative meridian plane fan passes the edge of the entrance pupil and is incident on the imaging plane at 0.7HOI. The lateral aberration is expressed as NSTA, and the longest working wavelength of the sagittal plane fan passes the edge of the entrance pupil and is incident on The lateral aberration at 0.7HOI on the imaging plane is expressed as SLTA, and the shortest operating wavelength of the sagittal plane fan passes through the edge of the entrance pupil and is incident on the imaging plane. The lateral aberration at 0.7HOI is expressed as SSTA, which satisfies the following conditions : PLTA ≦50 microns; PSTA≦50 microns; NLTA≦50 microns; NSTA≦50 microns; SLTA≦50 microns; and SSTA≦50 microns; |TDT|<150%. The optical imaging system according to claim 1, wherein the intersection of the object-side surface of the fifth lens on the optical axis is the starting point, and the contour of the surface is continued until the surface is perpendicular to the optical axis by 1/2 the diameter of the entrance pupil Up to the coordinate point at the height, the length of the contour curve between the aforementioned two points is ARE51, the intersection of the image side surface of the fifth lens on the optical axis is the starting point, and the contour of the surface is extended until the surface is 1/distance from the optical axis 2 Up to the coordinate point at the vertical height of the entrance pupil diameter, the length of the profile curve between the aforementioned two points is ARE52, and the thickness of the fifth lens on the optical axis is TP5, which satisfies the following conditions: 0.05≦ARE51/TP5≦15; and 0.05≦ARE52/TP5≦15. The optical imaging system according to claim 1, further comprising an aperture, and a distance InS on the optical axis from the aperture to the imaging plane, which satisfies the following formula: 0.2≦InS/HOS≦1.1. An optical imaging system includes, in order from the object side to the image side, a first lens made of glass and the object side and the image side are flat; a second lens with refractive power; a third lens with refractive power A fourth lens with refractive power; a fifth lens with refractive power; and an imaging surface, wherein the optical imaging system has five lenses with refractive power, the first lens to the fifth lens at least A lens has a positive refractive power, the material of the second lens to the fifth lens is plastic, the focal lengths of the first lens to the fifth lens are f1, f2, f3, f4, f5, respectively, the focal length of the optical imaging system Is f, the entrance pupil diameter of the optical imaging lens system is HEP, the first lens object side to the imaging plane has a distance HOS on the optical axis, the first lens object side to the fifth lens image side has a distance InTL on the optical axis, any of the lenses The intersection of any surface and the optical axis is the starting point, and the contour of the surface is continued until the coordinate point on the surface at a vertical height of 1/2 the entrance pupil diameter from the optical axis. The length of the contour curve between the two points is ARE , Which satisfies the following conditions: 1.0≦f/HEP≦10; 0.5≦HOS/f≦3; and 0.1≦2 (ARE/HEP)≦2.0. The optical imaging system according to claim 10, wherein half of the maximum viewing angle of the optical imaging lens system is HAF, which satisfies the following formula: 0deg<HAF≦50deg. The optical imaging system according to claim 10, wherein the thickness of the first lens is TP1 and the thickness of the third lens is TP3, which satisfies the following formula: TP1>TP3. The optical imaging system according to claim 10, wherein the distance between the third lens and the fourth lens on the optical axis is IN34, and the following formula is satisfied: 0.5mm≦IN34≦0.7mm. The optical imaging system according to claim 10, wherein the distance between the third lens and the fourth lens on the optical axis is IN34, and the distance between the fourth lens and the fifth lens on the optical axis is IN45, which satisfies the following formula: IN34>IN45. The optical imaging system according to claim 10, wherein the optical imaging system satisfies the following formula: f2>f3. The optical imaging system according to claim 10, wherein the maximum effective radius of any surface of any one of the lenses is expressed by EHD, and the The intersection of any surface of any lens and the optical axis of the lens is the starting point, and the contour of the surface is extended to the end of the maximum effective radius of the surface. The length of the contour curve between the two points is ARS, which satisfies the following formula: 0.9≦ARS/EHD≦2.0. The optical imaging system according to claim 10, wherein the visible light spectrum has a maximum imaging height HOI perpendicular to the optical axis on the imaging plane, and the longest working wavelength of the positive meridian plane fan of the optical imaging system passes through the entrance pupil edge The lateral aberration incident on the imaging plane at 0.7 HOI is expressed as PLTA, and the shortest operating wavelength of its positive meridian plane fan passes through the entrance pupil edge and is incident on the imaging plane. Indicates that the longest operating wavelength of the negative meridian plane fan passes the edge of the entrance pupil and is incident on the imaging plane at 0.7 HOI. The shortest operating wavelength of the negative meridian plane fan passes the entrance pupil edge The lateral aberration incident on the imaging plane at 0.7 HOI is expressed as NSTA, and the longest operating wavelength of the sagittal plane fan passes through the entrance pupil edge and is incident on the imaging plane. The lateral aberration incident on the imaging plane at 0.7 HOI is expressed as SLTA, arc The shortest operating wavelength of the sagittal fan passes through the edge of the entrance pupil and is incident on the imaging plane at 0.7HOI. The lateral aberration is expressed by SSTA, which satisfies the following conditions: PLTA≦100 microns; PSTA≦100 microns; NLTA≦100 microns; NSTA≦100 microns; SLTA≦100 microns; and SSTA≦100 microns. The optical imaging system according to claim 10, wherein the distance between the fourth lens and the fifth lens on the optical axis is IN45, and the following formula is satisfied: 0<IN45/f≦5.0. The optical imaging system according to claim 10, wherein the first lens, the second lens, the third lens, the fourth lens, and the fifth lens At least one of the lenses is a light filtering element with a wavelength less than 500nm. An optical imaging system includes, in order from the object side to the image side, a mechanism light entrance hole which restricts the path of light incident on the object side and has a diameter DDH; a first lens, which is made of glass and has an object side and an image The sides are all flat; a second lens with refractive power; a third lens with refractive power; a fourth lens with refractive power; a fifth lens with refractive power; and an imaging surface, wherein the second At least one lens from the lens to the fifth lens has a positive refractive power, the material of the second lens to the fifth lens is plastic, and the focal lengths of the first lens to the fifth lens are f1, f2, f3, f4, f5, the focal length of the optical imaging system is f, the entrance pupil diameter of the optical imaging lens system is HEP, the first lens object side to the imaging plane has a distance HOS on the optical axis, and the first lens object side to the The image side of the fifth lens has a distance InTL on the optical axis, the optical imaging system has a maximum imaging height HOI perpendicular to the optical axis on the imaging plane, and the intersection of any surface of any of the lenses with the optical axis As a starting point, the contour of the surface is continued until the coordinate point on the surface at a vertical height of 1/2 the entrance pupil diameter from the optical axis. The length of the contour curve between the two points is ARE, which satisfies the following conditions: 1.0≦f /HEP≦10; 0.5≦HOS/f≦3; 0mm<DDH≦10mm; and 0.1≦2 (ARE/HEP)≦2.0. The optical imaging system according to claim 20, wherein half of the maximum viewing angle of the optical imaging lens system is HAF, which satisfies the following Formula: 0deg<HAF≦50deg. The optical imaging system according to claim 20, wherein the distance between the center of the light inlet of the mechanism and the objective side center of the first lens on the optical axis is d, which satisfies the following formula: d≦1mm. The optical imaging system according to claim 20, wherein the refractive index of the first lens is Nd1, which satisfies the following formula: 1.70≦Nd1≦3.0. The optical imaging system according to claim 20, wherein the thickness of the first lens is TP1, which satisfies the following formula: 0.5mm≦TP1≦0.9mm. The optical imaging system according to claim 20, wherein the optical imaging system further includes an aperture, an image sensing element, and a driving module, the image sensing element is disposed on the imaging surface, and passes from the aperture to the imaging The surface has a distance InS on the optical axis. The driving module can couple with the lenses and cause the lenses to shift, which satisfies the following formula: 0.2≦InS/HOS≦1.1.

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