Patent Publication Number: US-10324275-B2

Title: Optical imaging lens

Description:
CROSS-REFERENCE TO RELATED APPLICATION 
     This application claims the priority benefit of Chinese application serial no. 201611253493.5, filed on Dec. 30, 2016. The entirety of the above-mentioned patent application is hereby incorporated by reference herein and made a part of this specification. 
     BACKGROUND OF THE INVENTION 
     1. Field of the Invention 
     The present invention relates to an optical lens, and particularly relates to an optical imaging lens. 
     In recent years, the popularization of portable electronic products such as mobile phones and digital cameras makes technologies related to an image module booming in development. The image module mainly contains components such as an optical imaging lens, a module holder unit (module holder unit), and a sensor (sensor). However, a trend that the mobile phones and the digital cameras become slimmer and lighter also makes requirements for miniaturization of the image module become higher. As development of technologies and miniaturization in size of a charge coupled device (charge coupled device, CCD) and a complementary metal oxide semiconductor (complementary metal oxide semiconductor, CMOS), the optical imaging lens installed in the image module also needs to be dwindled in size, but optical performances of the optical imaging lens should also be considered about. Using a seven-element lens structure as an example, a distance on an optical axis from an object-side surface of a first lens element to an image plane is great, and is detrimental to the thinning of the portable electronic products such as mobile phones and digital cameras. Therefore, an optical imaging lens having a good image quality, a large field of view, and a short system length is desired to be developed. 
     SUMMARY OF THE INVENTION 
     The invention is directed to an optical imaging lens, which still maintains good optical performance in case that a system length of the optical imaging lens is shortened. 
     An embodiment of the present invention provides an optical imaging lens including a first lens element, a second lens element, a third lens element, a fourth lens element, a fifth lens element, a sixth lens element, and a seventh lens element arranged in a sequence from an object side to an image side along an optical axis, wherein each of the first lens element to the seventh lens element has an object-side surface facing the object side and pervious to an imaging ray and an image-side surface facing the image side and pervious to the imaging ray. The object-side surface of the third lens element has a convex portion in a vicinity of a periphery. The object-side surface of the fifth lens element has a convex portion in a vicinity of the optical axis and a concave portion in a vicinity of a periphery. The object-side surface of the sixth lens element has a concave portion in a vicinity of a periphery. Lens elements having refracting power of the optical imaging lens are only the first lens element to the seventh lens element. 
     An embodiment of the present invention provides an optical imaging lens including a first lens element, a second lens element, a third lens element, a fourth lens element, a fifth lens element, a sixth lens element, and a seventh lens element arranged in a sequence from an object side to an image side along an optical axis, wherein each of the first lens element to the seventh lens element has an object-side surface facing the object side and pervious to an imaging ray and an image-side surface facing the image side and pervious to the imaging ray. The first lens element has positive refracting power. The object-side surface of the third lens element has a convex portion in a vicinity of a periphery. The object-side surface of the fifth lens element has a convex portion in a vicinity of the optical axis and a concave portion in the vicinity of the periphery. The image-side surface of the seventh lens element has a convex portion in a vicinity of a periphery. Lens elements having refracting power of the optical imaging lens are only the first lens element to the seventh lens element. 
     According to the above descriptions, advantageous effects of the optical imaging lens according to the embodiments of the invention are as follows. Based on the design and arrangement of the concave and convex shapes of the object-side surface or the image-side surface of the lens elements, the optical imaging lens is capable of providing good imaging quality in case that the system length of the optical imaging lens is shortened. 
     In order to make the aforementioned and other objectives and advantages of the present invention comprehensible, embodiments accompanied with figures are described in detail below. 
    
    
     
       BRIEF DESCRIPTION OF THE DRAWINGS 
       The accompanying drawings are included to provide a further understanding of the invention, and are incorporated in and constitute a part of this specification. The drawings illustrate embodiments of the invention and, together with the description, serve to explain the principles of the invention. 
         FIG. 1  is a schematic diagram illustrating a surface shape structure of a lens. 
         FIG. 2  is a schematic diagram illustrating surface shape concave and convex structures and a light focal point 
         FIG. 3  is a schematic diagram illustrating a surface shape structure of a lens of a first example. 
         FIG. 4  is a schematic diagram illustrating a surface shape structure of a lens of a second example. 
         FIG. 5  is a schematic diagram illustrating a surface shape structure of a lens of a third example. 
         FIG. 6  is a schematic diagram of an optical imaging lens according to a first embodiment of the present invention. 
         FIG. 7A  to  FIG. 7D  are various aberrations and a longitudinal spherical aberration of an optical imaging lens according to a first embodiment. 
         FIG. 8  shows detailed optical data of an optical imaging lens according to a first embodiment of the present invention. 
         FIG. 9  shows aspheric parameters of an optical imaging lens according to a first embodiment of the present invention. 
         FIG. 10  is a schematic diagram of an optical imaging lens according to a second embodiment of the present invention. 
         FIG. 11A  to  FIG. 11D  are various aberrations and a longitudinal spherical aberration of an optical imaging lens according to a second embodiment. 
         FIG. 12  shows detailed optical data of an optical imaging lens according to a second embodiment of the present invention. 
         FIG. 13  shows aspheric parameters of an optical imaging lens according to a second embodiment of the present invention. 
         FIG. 14  is a schematic diagram of an optical imaging lens according to a third embodiment of the present invention. 
         FIG. 15A  to  FIG. 15D  are various aberrations and a longitudinal spherical aberration of an optical imaging lens according to a third embodiment. 
         FIG. 16  shows detailed optical data of an optical imaging lens according to a third embodiment of the present invention. 
         FIG. 17  shows aspheric parameters of an optical imaging lens according to a third embodiment of the present invention. 
         FIG. 18  is a schematic diagram of an optical imaging lens according to a fourth embodiment of the present invention. 
         FIG. 19A  to  FIG. 19D  are various aberrations and a longitudinal spherical aberration of an optical imaging lens according to a fourth embodiment. 
         FIG. 20  shows detailed optical data of an optical imaging lens according to a fourth embodiment of the present invention. 
         FIG. 21  shows aspheric parameters of an optical imaging lens according to a fourth embodiment of the present invention. 
         FIG. 22  is a schematic diagram of an optical imaging lens according to a fourth embodiment of the present invention. 
         FIG. 23A  to  FIG. 23D  are various aberrations and a longitudinal spherical aberration of an optical imaging lens according to a fifth embodiment. 
         FIG. 24  shows detailed optical data of an optical imaging lens according to a fifth embodiment of the present invention. 
         FIG. 25  shows aspheric parameters of an optical imaging lens according to a fifth embodiment of the present invention. 
         FIG. 26  is a schematic diagram of an optical imaging lens according to a sixth embodiment of the present invention. 
         FIG. 27A  to  FIG. 27D  are various aberrations and a longitudinal spherical aberrations of an optical imaging lens according to a sixth embodiment. 
         FIG. 28  shows detailed optical data of an optical imaging lens according to a sixth embodiment of the present invention. 
         FIG. 29  shows aspheric parameters of an optical imaging lens according to a sixth embodiment of the present invention. 
         FIG. 30  is a schematic diagram of an optical imaging lens according to a seventh embodiment of the present invention. 
         FIG. 31A  to  FIG. 31D  are various aberrations and a longitudinal spherical aberration of an optical imaging lens according to a seventh embodiment. 
         FIG. 32  shows detailed optical data of an optical imaging lens according to a seventh embodiment of the present invention. 
         FIG. 33  shows aspheric parameters of an optical imaging lens according to a seventh embodiment of the present invention. 
         FIG. 34  is a schematic diagram of an optical imaging lens according to an eighth embodiment of the present invention. 
         FIG. 35A  to  FIG. 35D  are various aberrations and a longitudinal spherical aberrations of an optical imaging lens according to an eighth embodiment. 
         FIG. 36  shows detailed optical data of an optical imaging lens according to an eighth embodiment of the present invention. 
         FIG. 37  shows aspheric parameters of an optical imaging lens according to an eighth embodiment of the present invention. 
         FIG. 38  is a schematic diagram of an optical imaging lens according to a ninth embodiment of the present invention. 
         FIG. 39A  to  FIG. 39D  are various aberrations and a longitudinal spherical aberration of an optical imaging lens according to a ninth embodiment. 
         FIG. 40  shows detailed optical data of an optical imaging lens according to a ninth embodiment of the present invention. 
         FIG. 41  shows aspheric parameters of an optical imaging lens according to a ninth embodiment of the present invention. 
         FIG. 42  shows values of important parameters of an optical imaging lens according to first to ninth embodiments of the present invention. 
         FIG. 43  shows values of relational expressions of important parameters of an optical imaging lens according to first to ninth embodiments of the present invention. 
     
    
    
     DESCRIPTION OF THE EMBODIMENTS 
     In the present specification, the description “a lens element having positive refracting power (or negative refracting power)” means that the paraxial refracting power of the lens element in Gaussian optics is positive (or negative). The description “An object-side (or image-side) surface of a lens element” only includes a specific region of that surface of the lens element where imaging rays are capable of passing through that region, namely the clear aperture of the surface. The aforementioned imaging rays can be classified into two types, chief ray Lc and marginal ray Lm. Taking a lens element depicted in  FIG. 1  as an example, the lens element is rotationally symmetric, where the optical axis I is the axis of symmetry. The region A of the lens element is defined as “a portion in a vicinity of the optical axis”, and the region C of the lens element is defined as “a portion in a vicinity of a periphery of the lens element”. Besides, the lens element may also have an extending portion E extended radially and outwardly from the region C, namely the portion outside of the clear aperture of the lens element. The extending portion E is usually used for physically assembling the lens element into an optical imaging lens system. Under normal circumstances, the imaging rays would not pass through the extending portion E because those imaging rays only pass through the clear aperture. The structures and shapes of the aforementioned extending portion E are only examples for technical explanation, the structures and shapes of lens elements should not be limited to these examples. Note that the extending portions of the lens element surfaces depicted in the following embodiments are partially omitted. 
     The following criteria are provided for determining the shapes and the portions of lens element surfaces set forth in the present specification. These criteria mainly determine the boundaries of portions under various circumstances including the portion in a vicinity of the optical axis, the portion in a vicinity of a periphery of a lens element surface, and other types of lens element surfaces such as those having multiple portions. 
     1.  FIG. 1  is a radial cross-sectional view of a lens element. Before determining boundaries of those aforesaid portions, two referential points should be defined first, central point and transition point. The central point of a surface of a lens element is defined as a point of intersection of that surface and the optical axis. The transition point is defined as a point on a surface of a lens element, where the tangent line of that point is perpendicular to the optical axis. Additionally, if multiple transition points appear on one single surface, then these transition points are sequentially named along the radial direction of the surface with numbers starting from the first transition point. For instance, the first transition point (closest one to the optical axis), the second transition point, and the Nth transition point (farthest one to the optical axis within the scope of the clear aperture of the surface). The portion of a surface of the lens element between the central point and the first transition point is defined as the portion in a vicinity of the optical axis. The portion located radially outside of the Nth transition point (but still within the scope of the clear aperture) is defined as the portion in a vicinity of a periphery of the lens element. In some embodiments, there are other portions existing between the portion in a vicinity of the optical axis and the portion in a vicinity of a periphery of the lens element; the numbers of portions depend on the numbers of the transition point(s). In addition, the radius of the clear aperture (or a so-called effective radius) of a surface is defined as the radial distance from the optical axis I to a point of intersection of the marginal ray Lm and the surface of the lens element. 
     2. Referring to  FIG. 2 , determining the shape of a portion is convex or concave depends on whether a collimated ray passing through that portion converges or diverges. That is, while applying a collimated ray to a portion to be determined in terms of shape, the collimated ray passing through that portion will be bended and the ray itself or its extension line will eventually meet the optical axis. The shape of that portion can be determined by whether the ray or its extension line meets (intersects) the optical axis (focal point) at the object-side or image-side. For instance, if the ray itself intersects the optical axis at the image side of the lens element after passing through a portion, i.e. the focal point of this ray is at the image side (see point R in  FIG. 2 ), the portion will be determined as having a convex shape. On the contrary, if the ray diverges after passing through a portion, the extension line of the ray intersects the optical axis at the object side of the lens element, i.e. the focal point of the ray is at the object side (see point M in  FIG. 2 ), that portion will be determined as having a concave shape. Therefore, referring to  FIG. 2 , the portion between the central point and the first transition point has a convex shape, the portion located radially outside of the first transition point has a concave shape, and the first transition point is the point where the portion having a convex shape changes to the portion having a concave shape, namely the border of two adjacent portions. Alternatively, there is another common way for a person with ordinary skill in the art to tell whether a portion in a vicinity of the optical axis has a convex or concave shape by referring to the sign of an “R” value, which is the (paraxial) radius of curvature of a lens surface. The R value which is commonly used in conventional optical design software such as Zemax and CodeV. The R value usually appears in the lens data sheet in the software. For an object-side surface, positive R means that the object-side surface is convex, and negative R means that the object-side surface is concave. Conversely, for an image-side surface, positive R means that the image-side surface is concave, and negative R means that the image-side surface is convex. The result found by using this method should be consistent as by using the other way mentioned above, which determines surface shapes by referring to whether the focal point of a collimated ray is at the object side or the image side. 
     3. For none transition point cases, the portion in a vicinity of the optical axis is defined as the portion between 0˜50% of the effective radius (radius of the clear aperture) of the surface, whereas the portion in a vicinity of a periphery of the lens element is defined as the portion between 50˜100% of the effective radius (radius of the clear aperture) of the surface. 
     Referring to the first example depicted in  FIG. 3 , only one transition point, namely a first transition point, appears within the clear aperture of the image-side surface of the lens element. Portion I is a portion in a vicinity of the optical axis, and portion II is a portion in a vicinity of a periphery of the lens element. The portion in a vicinity of the optical axis is determined as having a concave surface due to that the R value at the image-side surface of the lens element is positive. The shape of the portion in a vicinity of a periphery of the lens element is different from that of the radially inner adjacent portion, i.e. the shape of the portion in a vicinity of a periphery of the lens element is different from the shape of the portion in a vicinity of the optical axis; the portion in a vicinity of a periphery of the lens element has a convex shape. 
     Referring to the second example depicted in  FIG. 4 , a first transition point and a second transition point exist on the object-side surface (within the clear aperture) of a lens element. In which portion I is the portion in a vicinity of the optical axis, and portion III is the portion in a vicinity of a periphery of the lens element. The portion in a vicinity of the optical axis has a convex shape because that the R value at the object-side surface of the lens element is positive. The portion in a vicinity of a periphery of the lens element (portion III) has a convex shape. What is more, there is another portion having a concave shape existing between the first and second transition points (portion II). 
     Referring to a third example depicted in  FIG. 5 , no transition point exists on the object-side surface of the lens element. In this case, the portion between 0˜50% of the effective radius (radius of the clear aperture) is determined as the portion in a vicinity of the optical axis, and the portion between 50˜100% of the effective radius is determined as the portion in a vicinity of a periphery of the lens element. The portion in a vicinity of the optical axis of the object-side surface of the lens element is determined as having a convex shape due to its positive R value, and the portion in a vicinity of a periphery of the lens element is determined as having a convex shape as well. 
       FIG. 6  is a schematic diagram of an optical imaging lens according to a first embodiment of the present invention.  FIG. 7A  to  FIG. 7D  are various aberrations and a longitudinal spherical aberration in a case in which a pupil radius is 1.4958 mm of an optical imaging lens according to the first embodiment. First, referring to  FIG. 6 , an optical imaging lens  10  of the first embodiment of the present invention includes an aperture stop  0 , a first lens element  1 , a second lens element  2 , a third lens element  3 , a fourth lens element  4 , a fifth lens element  5 , a sixth lens element  6 , a seventh lens element  7  and a light filter  9  arranged in a sequence from an object side to an image side along an optical axis I. An image is formed on an image plane  100  by rays emitted by an object and passed through the aperture stop  0 , the first lens element  1 , the second lens element  2 , the third lens element  3 , the fourth lens element  4 , the fifth lens element  5 , the sixth lens element  6 , the seventh lens element  7  and the light filter  9 . The light filter  9 , for example, is an IR cut filter, and is used to prevent infrared rays at some wave bands in the rays from being transmitted to the image plane  100  to affect an image quality. It is supplemented that the object side is a side facing the object to be shot, and the image side is a side facing the image plane  100 . 
     The first lens element  1 , the second lens element  2 , the third lens element  3 , the fourth lens element  4 , the fifth lens element  5 , the sixth lens element  6 , the seventh lens element land the light filter  9  respectively have object-side surfaces  11 ,  21 ,  31 ,  41 ,  51 ,  61 ,  71  and  91  facing the object side and pervious to imaging rays and image-side surfaces  12 ,  22 ,  32 ,  42 ,  52 ,  62 ,  72  and  92  facing the image side and pervious tothe imaging rays. 
     In addition, in order to satisfy requirements for light-weighting of products, the first lens element  1  to the seventh lens element  7  are all made of plastic materials, but materials of the first lens element  1  to the seventh lens element  7  still are not limited thereto. 
     The first lens element  1  has positive refracting power. The object-side surface  11  of the first lens element  1  is a convex surface, and has a convex portion  111  in a vicinity of the optical axis I and a convex portion  112  in a vicinity of a periphery. The image-side surface  12  of the first lens element  1  has a concave portion  121  in the vicinity of the optical axis I and a convex portion  122  in the vicinity of the periphery. In the present embodiment, the object-side surface  11  and the image-side surface  12  of the first lens element  1  both are aspheric surfaces. 
     The second lens element  2  has negative refracting power. The object-side surface  21  of the second lens element  2  has a convex portion  211  in a vicinity of the optical axis I and a concave portion  212  in a vicinity of the periphery. The image-side surface  22  of the second lens element  2  has a concave portion  221  in a vicinity of the optical axis I and a convex portion  222  in a vicinity of the periphery. In the present embodiment, the object-side surface  21  and the image-side surface  22  of the second lens element  2  both are aspheric surfaces. 
     The third lens element  3  has positive refracting power. The object-side surface  31  of the third lens element  3  has a convex portion  311  in a vicinity of the optical axis I and a convex portion  312  in a vicinity of the periphery. The image-side surface  32  of the third lens element  3  has a concave portion  321  in a vicinity of the optical axis I and a convex portion  322  in a vicinity of the periphery. In the present embodiment, the object-side surface  31  and the image-side surface  32  of the third lens element  3  both are aspheric surfaces. 
     The fourth lens element  4  has positive refracting power. The object-side surface  41  of the fourth lens element  4  has a concave portion  411  in a vicinity of the optical axis I and a concave portion  412  in a vicinity of the periphery. The image-side surface  42  of the fourth lens element  4  has a convex portion  421  in a vicinity of the optical axis I and a convex portion  422  in a vicinity of the periphery. In the present embodiment, the object-side surface  41  and the image-side surface  42  of the fourth lens element  4  both are aspheric surfaces. 
     The fifth lens element  5  has negative refracting power. The object-side surface  51  of the fifth lens element  5  has a convex portion  511  in a vicinity of the optical axis I and a concave portion  512  in a vicinity of the periphery. The image-side surface  52  of the fifth lens element  5  has a concave portion  521  in a vicinity of the optical axis I and a convex portion  522  in a vicinity of the periphery. In the present embodiment, the object-side surface  51  and the image-side surface  52  of the fifth lens element  5  both are aspheric surfaces. 
     The sixth lens element  6  has positive refracting power. The object-side surface  61  of the sixth lens element  6  has a convex portion  611  in a vicinity of the optical axis I and a concave portion  612  in a vicinity of the periphery. The image-side surface  62  of the sixth lens element  6  has a convex portion  621  in a vicinity of the optical axis I and a convex portion  622  in a vicinity of the periphery. In the present embodiment, the object-side surface  61  and the image-side surface  62  of the sixth lens element  6  both are aspheric surfaces. 
     The seventh lens element  7  has negative refracting power. The object-side surface  71  of the seventh lens element  7  has a concave portion  711  in a vicinity of the optical axis I and a concave portion  712  in a vicinity of the periphery. The image-side surface  72  of the seventh lens element  7  has a concave portion  721  in a vicinity of the optical axis I and a convex portion  722  in a vicinity of the periphery. In the present embodiment, the object-side surface  71  and the image-side surface  72  of the seventh lens element  7  both are aspheric surfaces. 
     In the present first embodiment, only the aforementioned lens elements has refracting power, and there are only seven lens elements having refracting power. 
     Other detailed optical data of the first embodiment is shown in  FIG. 8 . Moreover, in the first embodiment, an effective focal length EFL (effective focal length) of the optical imaging lens  10  is 4.487 mm, a half field of view HFOV (half field of view) is 36.052°, a system length TTL of the optical imaging lens  10  is 5.980 mm, and a f-number F NO  is 1.5. The system length TTL of the optical imaging lens  10  refers to a distance on the optical axis I from the object-side surface  11  of the first lens element  1  to the image plane  100 . 
     In addition, in the present embodiment, the object-side surfaces  11 ,  21 ,  31 ,  41 ,  51 ,  61  and  71  and the image-side surfaces  12 ,  22 ,  32 ,  42 ,  52 ,  62  and  72  of the first lens element  1 , the second lens element  2 , the third lens element  3 , the fourth lens element  4 , the fifth lens element  5 , the sixth lens element  6  and the seventh lens element  7  are all aspheric surfaces. Moreover, these aspheric surfaces are defined according to the following formula: 
     
       
         
           
             
               
                 
                   
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                           Y 
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                               1 
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                             2 
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                             i 
                           
                         
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     Wherein 
     Y: a distance between a point on an aspheric curve and the optical axis I; 
     Z: a depth of the aspheric surface (a perpendicular distance between the point on the aspheric surface that is spaced by the distance Y from the optical axis I and a tangent plane tangent to a vertex of the aspheric surface on the optical axis I); 
     R: a radius of curvature of the surface of the lens element; 
     K: a conic constant; 
     a 2i : 2i th  aspheric coefficient. 
     Aspheric constants in formula (1) from the object-side surface  11  of the first lens element  1  to the image-side surface  72  of the seventh lens element  7  are shown in  FIG. 9 . Number  11  in  FIG. 9  indicates that the number  11  is an aspheric constant of the object-side surface  11  of the first lens element  1 , and other numbers may be deduced by analogy. 
     In addition, key parameters and relationships between the key parameters of the optical imaging lens  10  of the first embodiment are shown in  FIG. 42  and  FIG. 43 . 
     Wherein, 
     T 1  is a center thickness of the first lens element  1  on the optical axis I; 
     T 2  is a center thickness of the second lens element  2  on the optical axis I; 
     T 3  is a center thickness of the third lens element  3  on the optical axis I; 
     T 4  is a center thickness of the fourth lens element  4  on the optical axis I; 
     T 5  is a center thickness of the fifth lens element  5  on the optical axis I; 
     T 6  is a center thickness of the sixth lens element  6  on the optical axis I; 
     T 7  is a center thickness of the seventh lens element  7  on the optical axis I; 
     G 12  is an air gap between the first lens element  1  and the second lens element  2  on the optical axis I; 
     G 23  is an air gap between the second lens element  2  and the third lens element  3  on the optical axis I; 
     G 34  is an air gap between the third lens element  3  and the fourth lens element  4  on the optical axis I; 
     G 45  is an air gap between the fourth lens element  4  and the fifth lens element  5  on the optical axis I; 
     G 56  is an air gap between the fifth lens element  5  and the sixth lens element  6  on the optical axis I; 
     G 67  is an air gap between the sixth lens element  6  and the seventh lens element  7  on the optical axis I; 
     G 7 F is an air gap between the seventh lens element  7  and the light filter  9  on the optical axis I; 
     AAG is a sum of six air gaps of the first lens element  1  to the seventh lens element  7  on the optical axis I; 
     ALT is a sum of center thicknesses of seven lenses from the first lens element  1  to the seventh lens element  7  on the optical axis I; 
     EFL is an effective focal length of the optical imaging lens  10 ; 
     BFL is a distance on the optical axis I from the image-side surface  72  of the seventh lens element  7  to the image plane  100 ; 
     TTL is a distance on the optical axis I from the object-side surface  11  of the first lens element  1  to the image plane  100 ; 
     TL is a distance on the optical axis I from the object-side surface  11  of the first lens element  1  to the image-side surface  72  of the seventh lens element  7 ; 
     Tmax is a maximum value of the center thicknesses of seven lenses from the first lens element  1  to the seventh lens element  7  on the optical axis I; 
     Tmin is a minimum value of the center thicknesses of the seven lenses from the first lens element  1  to the seventh lens element  7  on the optical axis I. 
     Reference is further made to  FIG. 7A  to  FIG. 7D .  FIG. 7A  and  FIG. 7B  respectively illustrate a field curvature aberration in a sagittal direction and a field curvature aberration in a tangential direction on the image plane  100  of the first embodiment.  FIG. 7C  illustrates a distortion aberration on the image plane  100  of the first embodiment.  FIG. 7D  illustrates a longitudinal spherical aberration of the first embodiment. 
     Referring to  FIG. 7A , in a diagram of a field curvature aberration in the sagittal direction of  FIG. 7A , focus variations of representative wavelengths of red, green, and blue of 650 nm, 555 nm and 470 nm within a range of an entire field of view fall within a range between −0.04-0.1 mm. Referring to  FIG. 7B , in a diagram of the field curvature aberration in the tangential direction of  FIG. 7B , focus variations of representative wavelengths of red, green, and blue of 650 nm, 555 nm and 470 nm within a range of an entire field of view fall within a range between −0.04-0.1 mm. It shows that an optical system of the first embodiment of the present invention can eliminate aberrations. Referring to  FIG. 7C , a distortion aberration diagram of  FIG. 7C  shows that a distortion aberration of the present first embodiment is maintained within a range between 0-25%, indicating that the distortion aberration of the present first embodiment satisfies the requirements for the image quality of the optical system. Referring to  FIG. 7D , in a diagram of longitudinal spherical aberrations in  FIG. 7D  according to the present first embodiment, curves of all wavelengths are close to each other and approach the middle, indicating that off-axis rays of different heights of each wavelength are converged nearby an imaging point. It can be seen from a deflection amplitude of a curve of each wavelength that a deviation of imaging points of the off-axis rays at different heights is controlled within a range from −0.01 mm to 0.014 mm. Therefore, the present embodiment obviously improves the aberration. In addition, distances between the representative wavelengths of red, green, and blue are also approximate to each other, this represents that imaging positions of rays of different wavelengths are quite converged. Therefore, chromatic aberration is also obviously improved. On this basis, as compared with an existing optical lens, the present first embodiment can still provide a better image quality under a condition that the TTL is shortened to be about 5.980 mm. Therefore, the present first embodiment can shorten a lens length while maintaining good optical performances. 
       FIG. 10  is a schematic diagram of an optical imaging lens according to a second embodiment of the present invention.  FIG. 11A  to  FIG. 11D  are various aberrations and a longitudinal spherical aberration in a case in which a pupil radius is 1.3983 mm of an optical imaging lens according to the second embodiment. First, referring to  FIG. 10 , the optical imaging lens  10  of the second embodiment of the present invention is substantially similar to the first embodiment, and is merely different in the optical data, the aspheric constants, and parameters between the first lens element  1 , the second lens element  2 , the third lens element  3 , the fourth lens element  4 , the fifth lens element  5 , the sixth lens element  6 , the seventh lens element  7  (for example, a radius of curvature, refracting power, center thickness, aspheric constants, or an EFL). Herein, it should be noted that in order to clearly show the diagram,  FIG. 10  omits some of numbers of concave portions and convex portions same to those in the first embodiment. 
     Detailed optical data of the optical imaging lens  10  according to the second embodiment is shown in  FIG. 12 . Moreover, in the second embodiment, an EFL is 4.195 mm, and an HFOV is 37.898°. A TTL of the optical imaging lens  10  according to the second embodiment is 5.771 mm, and an F NO  is 1.5. 
       FIG. 13  shows aspheric constants in formula (1) from the object-side surface  11  of the first lens element  1  to the image-side surface  72  of the seventh lens element  7  according to the second embodiment. 
     In addition, key parameters and relationships between the key parameters of the optical imaging lens  10  of the second embodiment are shown in  FIG. 42  and  FIG. 43 . 
     Referring to  FIG. 11A , in a diagram of a field curvature aberration in a sagittal direction of  FIG. 11A , focus variations of representative wavelengths of red, green, and blue within a range of an entire field of view fall within a range between −0.06-0.04 mm. Referring to  FIG. 11B , in a diagram of a field curvature aberration in a tangential direction of  FIG. 11B , focus variations of the representative wavelengths of red, green, and blue within the range of the entire field of view fall within a range between −0.065-0.06 mm. Referring to  FIG. 11C , a diagram of distortion aberrations in  FIG. 11C  shows that the distortion aberrations according to the present second embodiment are maintained within a range between 0-2.5%. Referring to  FIG. 11D , in a diagram of longitudinal spherical aberrations in  FIG. 11D  according to the present second embodiment, deviations of imaging points of off-axis rays of different heights are controlled within a range from −0.010 mm to 0.014 mm. On this basis, as compared with an existing optical lens, the present second embodiment can still provide a better image quality under a condition that the TTL is shortened to be about 5.771 mm. 
     It can be known from the foregoing description that the second embodiment has the following advantages as compared with the first embodiment: the TTL of the second embodiment is smaller than that of the first embodiment; the HFOV of the second embodiment is greater than that of first embodiment; and the field curvature aberration in the sagittal direction and the field curvature aberration in the tangential direction of the second embodiment are smaller than those of the first embodiment. 
       FIG. 14  is a schematic diagram of an optical imaging lens according to a third embodiment of the present invention.  FIG. 15A  to  FIG. 15D  are various aberrations and a longitudinal spherical aberration in a case in which a pupil radius is 0.9850 mm of an optical imaging lens according to the third embodiment. First, referring to  FIG. 14 , the optical imaging lens  10  of the third embodiment of the present invention is substantially similar to the first embodiment, and is merely different in the optical data, the aspheric constants, and parameters between the first lens element  1 , the second lens element  2 , the third lens element  3 , the fourth lens element  4 , the fifth lens element  5 , the sixth lens element  6 , the seventh lens element  7  (for example, a radius of curvature, refracting power, center thickness, aspheric constants, or a system focal length); and is different in that the image-side surface  12  of the first lens element  1  has a concave portion  122 ′ in a vicinity of a periphery, the object-side surface  41  of the fourth lens element  4  is a convex surface, the object-side surface  41  of the fourth lens element  4  has a convex portion  411 ′ in a vicinity of the optical axis and a convex portion  412 ′ in a vicinity of a periphery. Herein, it should be noted that in order to clearly show the diagram,  FIG. 14  omits numbers of the concave portions and the convex portions same to those in the first embodiment. 
     Detailed optical data of the optical imaging lens  10  according to the third embodiment is shown in  FIG. 16 . Moreover, in the third embodiment, an entire EFL is 2.955 mm, and an HFOV is 46.748°. A TTL of the optical imaging lens  10  according to the third embodiment is 5.842 mm, and an F NO  is 1.5. 
       FIG. 17  shows aspheric constants in formula (1) from the object-side surface  11  of the first lens element  1  to the image-side surface  72  of the seventh lens element  7  according to the third embodiment. 
     In addition, key parameters and relationships between the key parameters of the optical imaging lens  10  of the third embodiment are shown in  FIG. 42  and  FIG. 43 . 
     Referring to  FIG. 15A , in a diagram of a field curvature aberration in a sagittal direction of  FIG. 15A , focus variations of representative wavelengths of red, green, and blue within a range of an entire field of view fall within a range between −0.2-0.4 mm. Referring to  FIG. 15B , in a diagram of a field curvature aberration in the tangential direction of  FIG. 15B , focus variations of the representative wavelengths of red, green, and blue within the range of the entire field of view fall within a range between −0.2-0.12 mm. Referring to  FIG. 15C , a diagram of distortion aberrations in  FIG. 15C  shows that the distortion aberrations according to the present third embodiment are maintained within a range between 0-6%. Referring to  FIG. 15D , in a diagram of longitudinal spherical aberrations of  FIG. 15D  of the present third embodiment, a deviation of imaging points of off-axis rays of different heights is controlled within a range from −0.09 mm to 0 mm. On this basis, as compared with an existing optical lens, the present third embodiment can still provide a better image quality under a condition that the TTL is shortened to be about 5.842 mm. 
     It can be known from the foregoing description that the present third embodiment has the following advantages as compared with the first embodiment: the HFOV of the second embodiment is greater than the HFOV of first embodiment; and the TTL of the second embodiment is smaller than the TTL of the first embodiment. 
       FIG. 18  is a schematic diagram of an optical imaging lens according to a fourth embodiment of the present invention.  FIG. 19A  to  FIG. 19D  are various aberrations diagrams and longitudinal spherical aberrations in a case in which a pupil radius is 1.4050 mm of an optical imaging lens according to the fourth embodiment. First, referring to  FIG. 18 , the optical imaging lens  10  of the fourth embodiment of the present invention is substantially similar to the first embodiment, and is merely different in the optical data, the aspheric constants, and parameters between the first lens element  1 , the second lens element  2 , the third lens element  3 , the fourth lens element  4 , the fifth lens element  5 , the sixth lens element  6 , the seventh lens element  7  (for example, a radius of curvature, refracting power, center thickness, aspheric constants, or a system focal length); and is different in that the object-side surface  41  of the fourth lens element  4  has a convex portion  411 ′ in a vicinity of the optical axis, and the image-side surface  42  of the fourth lens element  4  has a concave portion  422 ′ in a vicinity of a periphery. Herein, it should be noted that in order to clearly show the diagram,  FIG. 18  omits numbers of the concave portion and the convex portion same to those in the first embodiment. 
     Detailed optical data of the optical imaging lens  10  according to the fourth embodiment is shown in  FIG. 20 . Moreover, in the fourth embodiment, an EFL is 4.215 mm, and an HFOV is 37.779°. A TTL of the optical imaging lens  10  according to the fourth embodiment is 5.793 mm, and an F NO  is 1.5. 
       FIG. 21  shows aspheric constants in formula (1) from the object-side surface  11  of the first lens element  1  to the image-side surface  72  of the seventh lens element  7  according to the fourth embodiment. 
     In addition, key parameters and relationships between the key parameters of the optical imaging lens  10  of the fourth embodiment are shown in  FIG. 42  and  FIG. 43 . 
     Referring to  FIG. 19A , in a diagram of a field curvature aberration in a sagittal direction of  FIG. 19A , focus variations of representative wavelengths of red, green, and blue within a range of an entire field of view fall within a range between −0.06-0.06 mm. Referring to  FIG. 19B , in a diagram of a field curvature aberration in a tangential direction of  FIG. 19B , focus variations of the representative wavelengths of red, green, and blue within the range of the entire field of view fall within a range between −0.06-0.14 mm. Referring to  FIG. 19C , a diagram of distortion aberrations in  FIG. 19C  shows that the distortion aberrations according to the present fourth embodiment are maintained within a range between 0-2.5%. Referring to  FIG. 19D , in a diagram of longitudinal spherical aberrations in  FIG. 11D  according to the present fourth embodiment, a deviation of imaging points of off-axis rays of different heights is controlled within a range from −0.008 mm to 0.014 mm. On this basis, as compared with the first embodiment, the present fourth embodiment can still provide a better image quality under a condition that the TTL is shortened to be about 5.793 nm. 
     It can be known from the foregoing description that the fourth embodiment has the following advantages as compared with the first embodiment: the HFOV of the fourth embodiment is greater than that of first embodiment; the TTL of the fourth embodiment is smaller than that of the first embodiment; the field curvature aberration in the sagittal direction of the fourth embodiment is smaller than that of the first embodiment; and the longitudinal spherical aberration of the fourth embodiment is smaller than that of the first embodiment. 
       FIG. 22  is a schematic diagram of an optical imaging lens according to a fifth embodiment of the present invention.  FIG. 23A  to  FIG. 23D  are aberration diagrams and a longitudinal spherical aberration in a case in which a pupil radius is 1.3738 mm of an optical imaging lens according to the fifth embodiment. First, referring to  FIG. 22 , the optical imaging lens  10  of the fifth embodiment of the present invention is substantially similar to the first embodiment, and is merely different in the optical data, the aspheric constants, and parameters between the first lens element  1 , the second lens element  2 , the third lens element  3 , the fourth lens element  4 , the fifth lens element  5 , the sixth lens element  6 , the seventh lens element  7  (for example, a radius of curvature, refracting power, center thickness, aspheric constants, or a system focal length); and is different in that the image-side surface  22  of the second lens element  2  has a concave portion  222 ′ in a vicinity of a periphery, and the object-side surface  41  of the fourth lens element  4  has a convex portion  411 ′ in a vicinity of the optical axis. Herein, it should be noted that in order to clearly show the diagram,  FIG. 22  omits numbers of the concave portion and the convex portion same to those in the first embodiment. 
     Detailed optical data of the optical imaging lens  10  according to the fifth embodiment is shown in  FIG. 24 . Moreover, in the fifth embodiment, an EFL is 4.122 mm, and an HFOV is 37.755°. A TTL of the optical imaging lens  10  according to the fifth embodiment is 5.738 mm, and an F NO  is 1.5. 
       FIG. 25  shows aspheric constants in formula (1) from the object-side surface  11  of the first lens element  1  to the image-side surface  72  of the seventh lens element  7  according to the fifth embodiment. 
     In addition, key parameters and relationships between the key parameters of the optical imaging lens  10  of the fifth embodiment are shown in  FIG. 42  and  FIG. 43 . 
     Referring to  FIG. 23A , in a diagram of a field curvature aberration in a sagittal direction of  FIG. 23A , focus variations of representative wavelengths of red, green, and blue within a range of an entire field of view fall within a range between −0.05-0.02 mm. Referring to  FIG. 23B , in a diagram of a field curvature aberration in a tangential direction of  FIG. 23B , focus variations of the representative wavelengths of red, green, and blue within the range of the entire field of view fall within a range between −0.06-0.07 mm. Referring to  FIG. 23C , a diagram of distortion aberrations in  FIG. 23C  shows that the distortion aberrations according to the present fifth embodiment are maintained within a range between 0-5%. Referring to  FIG. 23D , in a diagram of a longitudinal spherical aberration of  FIG. 23  of the present fifth embodiment, a deviation of imaging points of off-axis rays of different heights is controlled within a range from −0.006 mm to 0.012 mm. On this basis, as compared with an existing optical lens, the present fifth embodiment can still provide a better image quality under a condition that the TTL is shortened to be about 5.738 mm. 
     It can be known from the foregoing description that: the HFOV of the fifth embodiment is greater than that of first embodiment; the TTL of the fifth embodiment is smaller than that of the first embodiment; the field curvature aberration in the sagittal direction and the field curvature aberration in the tangential direction of the fifth embodiment are smaller than those of the first embodiment; and the longitudinal spherical aberration of the fifth embodiment is smaller than that of the first embodiment. 
       FIG. 26  is a schematic diagram of an optical imaging lens according to a sixth embodiment of the present invention.  FIG. 27A  to  FIG. 27D  are aberration diagrams and a longitudinal spherical aberration in a case in which a pupil radius is 1.4912 mm of an optical imaging lens according to the sixth embodiment. First, referring to  FIG. 26 , the optical imaging lens  10  of the sixth embodiment of the present invention is substantially similar to the first embodiment, and is merely different in the optical data, the aspheric constants, and parameters between the first lens element  1 , the second lens element  2 , the third lens element  3 , the fourth lens element  4 , the fifth lens element  5 , the sixth lens element  6 , the seventh lens element  7  (for example, a radius of curvature, refracting power, center thickness, aspheric constants, or a system focal length). Herein, it should be noted that in order to clearly show the diagram,  FIG. 26  omits some of numbers of the concave portion and the convex portion same to those in the first embodiment. 
     Detailed optical data of the optical imaging lens  10  according to the sixth embodiment is shown in  FIG. 28 . Moreover, in the sixth embodiment, an entire EFL is 4.474 mm, and an HFOV is 36.221°. A TTL of the optical imaging lens  10  according to the sixth embodiment is 5.980 mm, and an F NO  is 1.5. 
       FIG. 29  shows aspheric constants in formula (1) from the object-side surface  11  of the first lens element  1  to the image-side surface  72  of the seventh lens element  7  according to the sixth embodiment. 
     In addition, key parameters and relationships between the key parameters of the optical imaging lens  10  of the sixth embodiment are shown in  FIG. 42  and  FIG. 43 . 
     Referring to  FIG. 27A , in a diagram of a field curvature aberration in a sagittal direction of  FIG. 27A , focus variations of representative wavelengths of red, green, and blue within a range of an entire field of view fall within a range between −0.04-0.07 mm. Referring to  FIG. 27B , in a diagram of a field curvature aberration in a tangential direction of  FIG. 27B , focus variations of the representative wavelengths of red, green, and blue within the range of the entire field of view fall within a range between −0.05-0.06 mm. Referring to  FIG. 27C , a diagram of distortion aberrations in  FIG. 27C  shows that the distortion aberrations according to the present sixth embodiment are maintained within a range between 0-2%. Referring to  FIG. 27D , in a diagram of longitudinal spherical aberrations in  FIG. 27D  according to the present sixth embodiment, a deviation of imaging points of off-axis rays of different heights is controlled within a range from −0.006 mm to 0.019 mm. On this basis, as compared with the first embodiment, the present sixth embodiment can still provide a better image quality under a condition that the TTL is shortened to be about 5.980 mm. 
     It can be known from the foregoing description that the sixth embodiment has the following advantages as compared with the first embodiment: the HFOV of the sixth embodiment is greater than that of first embodiment; the field curvature aberration in the sagittal direction and the field curvature aberration in the tangential direction of the sixth embodiment are smaller than those of the first embodiment; and the TTL of the sixth embodiment is smaller than that of the first embodiment. 
       FIG. 30  is a schematic diagram of an optical imaging lens according to a seventh embodiment of the present invention.  FIG. 31A  to  FIG. 31D  are aberration diagrams and a longitudinal spherical aberration in a case in which a pupil radius is 1.4989 mm of an optical imaging lens according to the seventh embodiment. First, referring to  FIG. 30 , the optical imaging lens  10  of the third embodiment of the present invention is substantially similar to the first embodiment, and is merely different in the optical data, the aspheric constants, and parameters between the first lens element  1 , the second lens element  2 , the third lens element  3 , the fourth lens element  4 , the fifth lens element  5 , the sixth lens element  6 , the seventh lens element  7  (for example, a radius of curvature, refracting power, center thickness, aspheric constants, or a system focal length); and is different in that the image-side surface  12  of the first lens element  1  has a concave portion  122 ′ in a vicinity of a periphery, the image-side surface  22  of the second lens element  2  has a concave portion  222 ′ in a vicinity of a periphery, the image-side surface  32  of the third lens element  3  has a convex portion  321 ′ in a vicinity of the optical axis, and a portion in a vicinity of a periphery of the object-side surface  71  of the seventh lens element  7  has a convex portion  712 ′. Herein, it should be noted that in order to clearly show the diagram,  FIG. 30  omits numbers of the concave portions and the convex portions same to those in the first embodiment. 
     Detailed optical data of the optical imaging lens  10  according to the seventh embodiment is shown in  FIG. 32 . Moreover, in the seventh embodiment, an EFL is 4.497 mm, and an HFOV is 36.066°. A TTL of the optical imaging lens  10  according to the seventh embodiment is 5.989 mm, and an F NO  is 1.5. 
       FIG. 33  shows aspheric constants in formula (1) from the object-side surface  11  of the first lens element  1  to the image-side surface  72  of the seventh lens element  7  according to the seventh embodiment. 
     In addition, key parameters and relationships between the key parameters of the optical imaging lens  10  of the seventh embodiment are shown in  FIG. 42  and  FIG. 43 . 
     Referring to  FIG. 31A , in a diagram of a field curvature aberration in a sagittal direction of  FIG. 31A , focus variations of representative wavelengths of red, green, and blue within a range of an entire field of view fall within a range between −0.04-0.04 mm. Referring to  FIG. 31B , in a diagram of a field curvature aberration in a tangential direction of  FIG. 31B , focus variations of the representative wavelengths of red, green, and blue within the range of the entire field of view fall within a range between −0.06-0.12 mm. Referring to  FIG. 31C , a diagram of distortion aberrations in  FIG. 31C  shows that the distortion aberrations according to the present seventh embodiment are maintained within a range between 0-3.5%. Referring to  FIG. 31D , in a diagram of longitudinal spherical aberrations in  FIG. 31D  according to the present seventh embodiment, a deviation of imaging points of off-axis rays of different heights is controlled within a range from −0.01 mm to 0.025 mm. On this basis, as compared with an existing optical lens, the present seventh embodiment can still provide a better image quality under a condition that the TTL is shortened to be about 5.989 mm. 
     It can be known from the foregoing description that the seventh embodiment has the following advantage as compared with the first embodiment: the field curvature aberration in the sagittal direction of the seventh embodiment is smaller than that of the first embodiment. 
       FIG. 34  is a schematic diagram of an optical imaging lens according to an eighth embodiment of the present invention.  FIG. 35A  to  FIG. 35D  are aberration diagrams and a longitudinal spherical aberration in a case in which a pupil radius is 1.5153 mm of an optical imaging lens according to the eighth embodiment. First, referring to  FIG. 34 , the optical imaging lens  10  of the eighth embodiment of the present invention is substantially similar to the first embodiment, and is merely different in the optical data, the aspheric constants, and parameters between the first lens element  1 , the second lens element  2 , the third lens element  3 , the fourth lens element  4 , the fifth lens element  5 , the sixth lens element  6 , the seventh lens element  7  (for example, a radius of curvature, refracting power, center thickness, aspheric constants, or a system focal length); and is different in that the image-side surface  12  of the first lens element  1  has a concave portion  122 ′ in a vicinity of a periphery, the image-side surface  22  of the second lens element  2  has a concave portion  222 ′ in a vicinity of a periphery, the image-side surface  32  of the third lens element  3  has a convex portion  321 ′ in a vicinity of the optical axis, and the object-side surface  71  of the seventh lens element  7  has a convex portion  712 ′ in a vicinity of a periphery. Herein, it should be noted that in order to clearly show the diagram,  FIG. 34  omits some of numbers of the concave portions and the convex portions same to those in the eighth embodiment. 
     Detailed optical data of the optical imaging lens  10  according to the eighth embodiment is shown in  FIG. 36 . Moreover, in the eighth embodiment, an EFL is 4.546 mm, and an HFOV is 35.806°. A TTL of the optical imaging lens  10  according to the eighth embodiment is 6.001 mm, and an F NO  is 1.5. 
       FIG. 37  shows aspheric constants in formula (1) from the object-side surface  11  of the first lens element  1  to the image-side surface  72  of the seventh lens element  7  according to the eighth embodiment. 
     In addition, key parameters and relationships between the key parameters of the optical imaging lens  10  of the eighth embodiment are shown in  FIG. 42  and  FIG. 43 . 
     Referring to  FIG. 35A , in a diagram of a field curvature aberration in a sagittal direction of  FIG. 35A , focus variations of representative wavelengths of red, green, and blue within a range of an entire field of view fall within a range between −0.02-0.04 mm. Referring to  FIG. 35B , in a diagram of a field curvature aberration in a tangential direction of  FIG. 35B , focus variations of the representative wavelengths of red, green, and blue within the range of the entire field of view fall within a range between −0.06-0.16 mm. Referring to  FIG. 35C , a diagram of distortion aberrations in  FIG. 35C  shows that the distortion aberrations according to the present eighth embodiment are maintained within a range between 0-2.5%. Referring to  FIG. 35D , in a diagram of longitudinal spherical aberrations in  FIG. 35D  according to the present eighth embodiment, a deviation of imaging points of off-axis rays of different heights is controlled within a range from −0.005 mm to 0.025 mm. On this basis, as compared with an existing optical lens, the present eighth embodiment can still provide a better image quality under a condition that the TTL is shortened to be about 6.001 mm. 
     It can be known from the foregoing description that the eighth embodiment has the following advantage as compared with the first embodiment: the field curvature aberration in the sagittal direction of the eighth embodiment is smaller than that of the first embodiment. 
       FIG. 38  is a schematic diagram of an optical imaging lens according to a ninth embodiment of the present invention.  FIG. 39A  to  FIG. 39D  are aberration diagrams and a longitudinal spherical aberration in a case in which a pupil radius is 1.3562 mm of an optical imaging lens according to the ninth embodiment. First, referring to  FIG. 38 , the optical imaging lens  10  of the ninth embodiment of the present invention is substantially similar to the first embodiment, and is merely different in the optical data, the aspheric constants, and parameters between the first lens element  1 , the second lens element  2 , the third lens element  3 , the fourth lens element  4 , the fifth lens element  5 , the sixth lens element  6 , the seventh lens element  7  (for example, a radius of curvature, refracting power, center thickness, aspheric constants, or a system focal length); and is different in that the image-side surface  52  of the fifth lens element  5  has a concave portion  522 ′ in a vicinity of a periphery. Herein, it should be noted that in order to clearly show the diagram,  FIG. 38  omits some of numbers of concave portions and convex portions same to those in the first embodiment. 
     Detailed optical data of an optical imaging lens  10  according to the ninth embodiment is shown in  FIG. 40 . Moreover, in the ninth embodiment, an EFL is 4.069 mm, and an HFOV is 38.954°. A TTL of the optical imaging lens  10  according to the ninth embodiment is 5.763 mm, and an F NO  is 1.5. 
       FIG. 41  shows aspheric constants in formula (1) from the object-side surface  11  of the first lens element  1  to the image-side surface  72  of the seventh lens element  7  according to the ninth embodiment. 
     In addition, key parameters and relationships between the key parameters of the optical imaging lens  10  of the ninth embodiment are shown in  FIG. 42  and  FIG. 43 . 
     Referring to  FIG. 39A , in a diagram of a field curvature aberration in a sagittal direction of  FIG. 39A , focus variations of representative wavelengths of red, green, and blue within a range of an entire field of view fall within a range between −0.04-0.06 mm. Referring to  FIG. 39B , in a diagram of a field curvature aberration in a tangential direction of  FIG. 39B , focus variations of the representative wavelengths of red, green, and blue within the range of the entire field of view fall within a range between −0.06-0.12 mm. Referring to  FIG. 39C , a diagram of distortion aberrations in  FIG. 39C  shows that the distortion aberrations according to the present ninth embodiment are maintained within a range between −1-2.5%. Referring to  FIG. 39D , in a diagram of  FIG. 39D  of longitudinal spherical aberrations according to the present ninth embodiment, a deviation of imaging points of off-axis rays of different heights is controlled within a range from −0.005 mm to 0.035 mm. On this basis, as compared with an existing optical lens, the present ninth embodiment can still provide a better image quality under a condition that a TTL is shortened to be about 5.763 mm. 
     It can be known from the foregoing description that the ninth embodiment has the following advantages as compared with the first embodiment: the HFOV of the ninth embodiment is greater than that of first embodiment; the TTL of the ninth embodiment is smaller than that of the first embodiment; and the field curvature aberration in the sagittal direction of the ninth embodiment is smaller than that of the first embodiment. 
     In at least one of the foregoing embodiments from the first embodiment to the ninth embodiment, the first lens element has positive refracting power and therefore has good light converging effect; the object-side surface of the third lens element is designed to have a convex portion in a vicinity of a periphery, and the object-side surface of the fifth lens element is designed to have a convex portion in a vicinity of the optical axis and a concave portion in the vicinity of the periphery; and in addition, the object-side surface of the sixth lens element has a concave portion in a vicinity of the periphery, or the image-side surface of the seventh lens element comprises a convex portion in a vicinity of the periphery, which has good effects on correcting an aberration. 
     Subsequently,  FIG. 43  is a table of optical parameters in the foregoing embodiments from the first embodiment to the ninth embodiment. When relational expressions between the optical parameters in the optical imaging lens  10  of the embodiments of the present invention satisfy at least one of the following conditional expressions, a designer may be assisted to design an optical imaging lens which has good optical performances and an effectively shortened TTL, and is technically practicable: 
     I. When the optical imaging lens of the embodiments of the present invention satisfies any one of the following conditional expressions, an effect of shortening the TTL is achieved by reducing an air gap between lens elements or shortening thickness of a lens element, and meanwhile considering the difficulty for manufacturing: ALT/(T 3 +T 4 )≤4.0; AAG/(G 12 +G 34 )≤3.6; TTL/EFL≤2.5; AAG/(G 34 +G 67 )≤3.0; Tmax/Tmin≤3.0; TL/(T 1 +T 3 +T 6 )≤3.0; (T 1 +T 6 )/(T 2 +T 5 )≥1.7; (G 67 +T 7 )/(T 4 +G 45 )≤2.1; EFL/T 3 ≤8.5; (ALT+AAG)/EFL≤2.1; (T 1 +T 2 +T 3 )/T 7 ≥2.8; AAG/(G 34 +G 56 )≤2.8; (T 6 +G 67 )/T 5 ≥2.0; (G 34 +T 4 )/(G 12 +T 2 )≥1.8; (T 3 +T 4 )/G 34 ≤3 0.7; EFL/T 1 ≥3; or (T 3 +G 34 )/T 2 ≥2.5. 
     II. When the optical imaging lens of the present invention satisfies any one of the following conditional expressions, it indicates that the optical imaging lens has a better configuration and can generate a good image quality on the premise of ensuring appropriate yield: 2.5≤ALT/(T 3 +T 4 )≤4.0; 2.0≤AAG/(G 12 +G 34 )≤3.6; 1.0≤TTL/EFL≤2.5; 1.0≤AAG/(G 34 +G 67 )≤3.0; 2.2≤Tmax/Tmin≤3.0; 2.0≤TL/(T 1 +T 3 +T 6 )≤3.0; 3.0≥(T 1 +T 6 )/(T 2 +T 5 )≥1.7; 0.5≤(G 67 +T 7 )/(T 4 +G 45 )≤2.1; 4.3≤EFL/T 3 ≤8.5; 1.0≤(ALT+AAG)/EFL≤2.1; 6.0≥(T 1 +T 2 +T 3 )/T 7 ≥2.8; 1.5≤AAG/(G 34 +G 56 )≤2.8; 4.7≥(T 6 +G 67 )/T 5 ≥2.0; 3.1≥(G 34 +T 4 )/(G 12 +T 2 )≥1.8; 2.0≤(T 3 +T 4 )/G 34 ≤3.7; 6.8≥EFL/T 1 ≥3; 4.0≥(T 3 +G 34 )/T 2 ≥2.5. 
     However, considering unpredictability of design of an optical system, under an architecture of the embodiments of the present invention, satisfying the foregoing conditional expressions can better shorten a lens length of the lens of the present invention, may enlarge an available aperture stop, increase a field of view, improve an image quality, or improve assembling yield, so that disadvantages of the prior art are improved. 
     Based on the above, the optical imaging lens  10  of the embodiments of the present invention may have the following effects and advantages: 
     The longitudinal spherical aberrations, astigmatic aberrations, and distortions of the embodiments of the present invention all meet usage specifications. In addition, off-axis rays at different heights of the representative wavelengths of red, green, and blue are all converged nearby an imaging point. It can be seen from a deflection amplitude of each curve that deviations of imaging points of the off-axis rays at different heights are all controlled to have good spherical aberrations, aberrations, and distortion inhibiting capabilities. Further referring to data of the image quality, distances between the representative wavelengths of red, green, and blue are also approximate to each other, indicating that the present invention, under different statuses, has good convergence for rays of different wavelength, so as to have a good dispersion inhibiting capability. Based on the above, the present invention can generate an excellent image quality via the design and association of the lens. 
     Although the present invention discloses the foregoing by using the embodiment, the foregoing is not intended to limit the present invention. Any person of ordinary skill in the art may make some variations and modifications without departing from the scope and spirit of the invention. Therefore, the protection scope of the present invention should fall within the scope defined by the appended claims below.