Abstract:
An optical lens system for taking image comprises three lens elements with refractive power, from the object side to the image side: a first lens element with positive refractive power having a convex object-side surface and a convex image-side surface, and the object-side surface being aspheric; a plastic second lens element with negative refractive power having a concave object-side surface and a convex image-side surface, and the front and image-side surfaces thereof being aspheric; a plastic third lens element with positive refractive power having a convex object-side surface and a concave image-side surface, the front and image-side surfaces thereof being aspheric; wherein an aperture stop is located between the first and second lens elements. By such arrangements, it can reduce the volume and sensitivity of the optical lens system, and furthermore can obtain higher resolution.

Description:
BACKGROUND OF THE INVENTION 
       [0001]    1. Field of the Invention 
         [0002]    The present invention relates to an optical lens system, and more particularly to a miniaturized optical lens system for taking image used in a camera mobile phone. 
         [0003]    2. Description of the Prior Art 
         [0004]    In recent years, with the popularity of camera mobile phone, the optical lens system for taking image has been becoming thinner and thinner, and the sensor of a general digital camera is none other than CCD (Charge Coupled Device) or CMOS (Complementary Metal Oxide Semiconductor). Due to advances in semiconductor manufacturing, the pixel size of sensor has been being reduced continuously, and miniaturized optical lens systems for taking image have increasingly higher resolution. Therefore, the demand for the image quality becomes increasingly urgent. 
         [0005]    A conventional mobile phone&#39;s lens assembly usually consists of three lens elements: from the object side to the image side: a first lens element with positive refractive power, a second lens element with negative refractive power and a third lens element with positive refractive power, thus forming the so-called type of Triplet. To correct the aberration, the optical lens system usually takes the form of “front aperture stop”. However, the arrangement of front aperture stop will increase the occurrence of stray light and the sensitivity of the optical lens system. 
         [0006]    The present invention mitigates and/or eliminates the afore-described disadvantages. 
       SUMMARY OF THE INVENTION 
       [0007]    The primary objective of the present invention is to improve the image quality and effectively reduce the volume of the optical lens system. The present invention provides a whole new three-lens type optical lens system. 
         [0008]    An optical lens system for taking image in accordance with the present invention comprises three lens elements with refractive power, from the object side to the image side: 
         [0009]    a first lens element with positive refractive power having a convex object-side surface and a convex image-side surface, and the object-side surface of the first lens element being aspheric; 
         [0010]    a plastic second lens element with negative refractive power having a concave object-side surface and a convex image-side surface, and the front and image-side surfaces of the second lens element being aspheric; 
         [0011]    a plastic third lens element with positive refractive power having a convex object-side surface and a concave image-side surface, the front and image-side surfaces of the third lens element being aspheric; 
         [0012]    wherein an aperture stop of the optical lens system is located between the first and second lens elements. 
         [0013]    In the present optical lens system for taking image, the object-side surface and the image-side surface of the first lens element with positive refractive power are convex. The object-side surface and the image-side surface of the second lens element with negative refractive power are concave and convex, respectively. And the object-side surface and the image-side surface of the third lens element with positive refractive power are convex and concave, respectively. By such arrangements, the image quality can be improved effectively. 
         [0014]    An electronic sensor is disposed in the optical lens system, and an object to be photographed is imaged on the electronic photosensitive assembly. The first lens element provides a positive refractive power, and the aperture stop is located close to the object side, so that the exit pupil of the optical lens system will be far away from the image plane. Therefore, the light will be projected onto the sensor with a relatively small incident angle, this is the telecentric feature of the image side, and this feature is very important to the photosensitive power of the current solid-state sensor, and can improve the photosensitivity of the sensor while reducing the probability of the occurrence of vignetting. And at least one inflection point is formed on the third lens element to making it easier for the optical designer to control light&#39;s incident angle on the sensor. In addition, for a wide-angle optical lens system, it particularly needs to correct the distortion and the chromatic aberration of magnification, the correction method is to arrange the aperture stop at the balance point of the refractive power of the optical lens system. And the aperture stop of the optical lens system of the present invention is located between the first lens element and the second lens element, the purpose of such an arrangement is to balance the telecentric and wide field of view. Further, the position of the aperture stop can effectively reduce the refraction angle of the light with respect to the lens element, thus reducing the sensitivity of the optical lens system. 
         [0015]    With the trend of miniaturization of the optical lens system and the requirement of increasing the field of view, the focal length of the optical lens system is becoming very short. Therefore, the radius of curvature and the size of the lens elements must be very small, and it is impossible to make such glass lens elements by the use of the conventional grind method. Plastic material is introduced to make lens elements by injection molding, using a relatively low cost to produce high precision lens elements. The surface of lens element is aspheric for allowing more design parameters (than spherical surfaces), so as to better reduce the aberration and the number of the lens elements, so that the length of the optical lens system can be reduced effectively. 
         [0016]    In the present optical lens system for taking image, an Abbe number of the second lens element is V2, and it satisfies the relation: 
         [0000]      V2&lt;40 
         [0017]    The above relation can effectively correct the chromatic aberration caused by the system, and improve the resolution of the optical lens system for taking image. 
         [0018]    And it will be better if the Abbe number V2 of the second lens element satisfies the relation: 
         [0000]      V2&lt;28 
         [0019]    And it will be much better if the Abbe number V2 of the second lens element satisfies the relation: 
         [0000]      V2&lt;25 
         [0020]    In the present optical lens system for taking image, the refractive index of the first lens element is N1, the refractive index of the second lens element is N2, and they satisfy the relations: 
         [0000]      N1&lt;1.6 
         [0000]      N2&lt;1.75 
         [0021]    If the refractive indexes of the first and second lens elements are higher than the high limit as stated above, it will be difficult to find an appropriate plastic optical material to match the optical lens system. 
         [0022]    And it will be better if the refractive index of the second lens element satisfies the relation: 
         [0000]      N2&lt;1.65 
         [0023]    In the present optical lens system for taking image, the radius of curvature of the object-side surface of the first lens element is R1, the radius of curvature of the image-side surface of the first lens element is R2, and they satisfy the relation: 
         [0000]      0.01 &lt;|R 1 /R 2|&lt;0.35 
         [0024]    If the value of R1/R2 is lower than the low limit as stated above, it will be difficult to correct the astigmatism caused by the optical lens system for taking image. On the other hand, if the value of R1/R2 is higher than the above high limit, it will be difficult to correct the spherical aberration caused by the optical lens system. And it will be better if the value of R1/R2 satisfies the relation: 
         [0000]      0.03 &lt;|R 1 /R 2|&lt;0.18 
         [0025]    In the present optical lens system for taking image, the radius of curvature of the object-side surface of the second lens element is R3, the radius of curvature of the image-side surface of the second lens element is R4, and they satisfy the relation: 
         [0000]      0.45 &lt;R 3 /R 4&lt;0.6 
         [0026]    If the value of R3/R4 is lower than the low limit as stated above, R3 will be smaller, and the length of the optical lens system for taking image will be too long. On the other hand, if the value of R3/R4 is higher than the high limit as stated above, R3 will be relatively large, and the chromatic aberration caused by the optical lens system for taking image will become difficult to correct. 
         [0027]    In the present optical lens system for taking image, the radius of curvature of the object-side surface of the third lens element is R5, the radius of curvature of the image-side surface of the third lens element is R6, and they satisfy the relation: 
         [0000]      0.3 &lt;R 5 /R 6&lt;0.45 
         [0028]    The above relation can effectively correct the high order aberration of the optical lens system for taking image. 
         [0029]    In the present optical lens system for taking image, the center thickness of the second lens element is CT2, and it satisfies the relation: 
         [0000]      0.25 mm&lt;CT2&lt;0.4 mm 
         [0030]    If the value of CT2 is lower than the high limit as stated above, it can reduce the length of the optical lens system while improving the image quality effectively. If the value of CT2 is higher than the low limit as stated above, the plastic lens elements made by injection molding will be more homogeneous in material properties. 
         [0031]    In the present optical lens system for taking image, the distance between the second lens element and the third lens element is T23, and it satisfies the relation: 
         [0000]      T23&gt;0.25 mm 
         [0032]    The relation as stated above can effectively correct the high order aberration of the optical lens system for taking image. 
         [0033]    In the present optical lens system for taking image, the focal length of the first lens element is f1, the focal length of the optical lens system is f, and they satisfy the relation: 
         [0000]        f/f 1&gt;0.95 
         [0034]    If the value of f/f1 is smaller than the above low limit, the refractive power of the optical lens system for taking image will be weak, the length of the optical lens system for taking image will be too long, and it will be difficult to suppress the incident angle of light to the photosensitive assembly. Further, it will be better if the value of f/f1 satisfies the relation: 
         [0000]        f/f 1&gt;1.22 
         [0035]    In the present optical lens system for taking image, the focal length of the second lens element is f2, the focal length of the optical lens system is f, and they satisfy the relation: 
         [0000]      0.7 &lt;|f/f 2|&lt;1.4 
         [0036]    If the value of |f/f2| is smaller than the above low limit, it will be difficult to correct the chromatic aberration caused by the optical lens system, and if the value of |f/f2| is greater than the above high limit, the length of the optical lens system for taking image will be too long, and this will be counter to the objective of miniaturization of the optical lens system for taking image. 
         [0037]    In the present optical lens system for taking image, the focal length of the third lens element is f3, the focal length of the optical lens system is f, and they satisfy the relation: 
         [0000]        f/f 3&gt;0.7 
         [0038]    If the value of f/f3 is smaller than the above low limit, the back focal length of the optical lens system will be too long. 
         [0039]    In the present optical lens system for taking image, the radius of curvature of the object-side surface of the first lens element is R1, and it satisfies the relation: 
         [0000]      R1&lt;2.3 mm 
         [0040]    The above relation can effectively improve refractive power of the first lens element and reduce the length of the optical lens system for taking image. 
         [0041]    It will be better if R1 satisfies the relation: 
         [0000]        R 1/ f&lt; 0.52 
         [0042]    In the present optical lens system for taking image, the radius of curvature of the object-side surface of the second lens element is R3, and it satisfies the relation: 
         [0000]      | R 3|&lt;1.0 mm 
         [0043]    The above relation can effectively correct the chromatic aberration caused by the optical lens system. 
         [0044]    It will be better if R3 satisfies the relation: 
         [0000]      | R 3 /f |&lt;0.23 
         [0045]    In the present optical lens system for taking image, an object to be photographed is imaged on an electronic sensor, a length of the optical lens system is TL, an image height of the optical lens system is ImgH, and they satisfy the relation: 
         [0000]        TL/ImgH&lt; 2.05 
         [0046]    The above relation contributes to the miniaturization of the optical lens system for taking image. 
         [0047]    In the present optical lens system for taking image, the chief ray angle of the maximal field of view is CRA, half of the maximal field of view is HFOV, and they satisfy the relation: 
         [0000]      0.45&lt;(tan(CRA))/(tan(HFOV))&lt;1.15 
         [0048]    The above relation makes the optical lens system compatible with the electronic sensor, and enables the optical system for taking image to have a wide field of view. 
     
    
     
       BRIEF DESCRIPTION OF THE DRAWINGS 
         [0049]      FIG. 1  shows an optical lens system for taking image in accordance with a first embodiment of the present invention; 
           [0050]      FIG. 2  shows the aberration curve of the first embodiment of the present invention; 
           [0051]      FIG. 3  shows an optical lens system for taking image in accordance with a second embodiment of the present invention; and 
           [0052]      FIG. 4  shows the aberration curve of the second embodiment of the present invention. 
       
    
    
     DETAILED DESCRIPTION OF THE PREFERRED EMBODIMENTS 
       [0053]    Referring to  FIG. 1 , which shows an optical lens system for taking image in accordance with a first embodiment of the present invention, and  FIG. 2  shows the aberration curve of the first embodiment of the present invention. The first embodiment of the present invention is an optical lens system for taking image comprising three lens elements with refractive power. An electronic sensor is disposed in the optical lens system, and an object to be photographed is imaged on an electronic photosensitive assembly. The optical lens system for taking image comprises: from the object side to the image side: 
         [0054]    A plastic first lens element  10  with positive refractive power has a convex object-side surface  11  and a convex image-side surface  12 , and the object-side surface  11  and the image-side surface  12  of the first lens element  10  are aspheric. 
         [0055]    A plastic second lens element  20  with negative refractive power has a concave object-side surface  21  and a convex image-side surface  22 , and the object-side surface  21  and the image-side surface  22  of the second lens element  20  are aspheric. 
         [0056]    A plastic third lens element  30  with positive refractive power has a convex object-side surface  31  and a concave image-side surface  32 , the object-side surface  31  and the image-side surface  32  of the third lens element  30  are aspheric, and each of the two surfaces is formed with an inflection point. 
         [0057]    An aperture stop  40  is located between the first lens element  10  and the second lens element  20 . 
         [0058]    An IR cut filter  50  is located behind the third lens element  30  and has no influence on the focal length of the optical lens system. 
         [0059]    A sensor cover glass  60  is located behind the IR cut filter  50  and has no influence on the focal length of the optical lens system. 
         [0060]    An image plane  70  is located behind the sensor cover glass  60 . 
         [0061]    The equation of the curve of the aspheric surfaces is expressed as follows: 
         [0000]        X ( Y )=( Y   2   /R )/(1+ sqrt (1−(1+ k )*( Y/R ) 2 ))+ A   4   *Y   4   +A   6   *Y   6 + . . . 
         [0062]    wherein: 
         [0063]    X: the length of a line drawn from a point on the aspheric lens surface at a distance Y from the optical axis to the tangential plane of the aspheric surface vertex; 
         [0064]    Y: the distance from the point on the curve of the aspheric surface to the optical axis; 
         [0065]    K: represents the conic coefficient; 
         [0066]    A 4 , A 6  . . . : the aspheric surface coefficients of the fourth order, sixth order, . . . 
         [0067]    In the present optical lens system for taking image of the first embodiment, the Abbe number of the second lens element is V2, and it satisfies the relation: V2=30.2. 
         [0068]    In the first embodiment of the optical lens system for taking image, the refractive index of the first lens element is N1, and the refractive index of the second lens element is N2, and they satisfy the relations: N1=1.543, N2=1.583. 
         [0069]    In the first embodiment of the optical lens system for taking image, the radius of curvature of the object-side surface of the first lens element is R1, the radius of curvature of the image-side surface of the first lens element is R2, the radius of curvature of the object-side surface of the second lens element is R3, the radius of curvature of the image-side surface of the second lens element is R4, the radius of curvature of the object-side surface of the third lens element is R5, the radius of curvature of the image-side surface of the third lens element is R6, they satisfy the relations: |R1R2|=0.16, R3/R4=0.47, R5/R6=0.35. 
         [0070]    In the first embodiment of the optical lens system for taking image, the focal length of the first lens element is f1, the focal length of the second lens element is f2, the focal length of the third lens element is f3, the focal length of the optical lens system for taking image is f, and they satisfy the relations: f/f1=1.27, |f/f2|=1.34, f/f3=1.02. 
         [0071]    In the first embodiment of the optical lens system for taking image, the center thickness of the second lens element is CT2, the distance between the second lens element and the third lens element is T23, and they satisfy the relations: CT2=0.412 mm, T23=0.372 mm. 
         [0072]    In the first embodiment of the optical lens system for taking image, the radius of curvature of the object-side surface of the first lens element is R1, the radius of curvature of the object-side surface of the second lens element is R3, the focal length of the optical lens system for taking image is f, and they satisfy the relations: R1=2.17692 mm, |R3|=0.86293 mm, R1/f=0.49, |R3/f|=0.19. 
         [0073]    In the first embodiment of the optical lens system for taking image, the length of the optical lens system is TL, the image height of the optical lens system is ImgH, and they satisfy the relation: TL/ImgH=1.98. 
         [0074]    In the first embodiment of the optical lens system for taking image, the chief ray angle of the maximal field of view is CRA, half of the maximal field of view is HFOV, and they satisfy the relation: 
         [0000]      (tan(CRA))/(tan(HFOV))=0.62. 
         [0075]    The detailed optical data the structure of the first embodiment is shown in table 1, and the aspheric surface data is shown in table 2, wherein the units of the radius of curvature, the thickness and the focal length are expressed in mm, and HFOV is half of the maximal field of view. 
         [0000]    
       
         
               
             
               
               
               
               
               
               
               
               
             
               
               
               
               
               
               
               
               
             
           
               
                 TABLE 1 
               
             
             
               
                   
               
               
                 (Embodiment 1) 
               
               
                 f(focal length) = 4.46 mm, Fno = 3.2, HFOV (half of field of view) = 33.4 deg. 
               
             
          
           
               
                   
                   
                 Curvature 
                   
                   
                   
                   
                 Focal 
               
               
                 Surface # 
                   
                 Radius 
                 Thickness 
                 Material 
                 Index 
                 Abbe # 
                 length 
               
               
                   
               
             
          
           
               
                 0 
                 Object 
                 Plano 
                 Infinity 
                   
                   
                   
                   
               
               
                 1 
                 Lens 1 
                 2.17692(ASP) 
                 0.695 
                 Plastic 
                 1.543 
                 60.3 
                 3.51 
               
               
                 2 
                   
                 −13.65360(ASP)  
                 0.029 
               
               
                 3 
                 Ape. 
                 Plano 
                 0.790 
               
               
                   
                 Stop 
               
               
                 4 
                 Lens 2 
                 −0.86293(ASP)  
                 0.412 
                 Plastic 
                 1.583 
                 30.2 
                 −3.33 
               
               
                 5 
                   
                 −1.82560(ASP)  
                 0.372 
               
               
                 6 
                 Lens 3 
                 1.69512(ASP) 
                 1.200 
                 Plastic 
                 1.53 
                 55.8 
                 4.34 
               
               
                 7 
                   
                 4.85580(ASP) 
                 0.200 
               
               
                 8 
                 IR-filter 
                 Plano 
                 0.300 
                 Glass 
                 1.517 
                 64.1 
                 — 
               
               
                 9 
                   
                 Plano 
                 0.500 
               
               
                 10 
                 Cover 
                 Plano 
                 0.500 
                 Glass 
                 1.517 
                 64.1 
                 — 
               
               
                   
                 Glass 
               
               
                 11 
                   
                 Plano 
                 0.832 
               
               
                 12 
                 Image 
                 Plano 
               
               
                   
               
             
          
         
       
     
         [0000]    
       
         
               
             
               
               
             
               
               
               
               
               
               
               
             
               
               
               
               
               
               
               
             
           
               
                 TABLE 2 
               
             
             
               
                   
               
               
                 Aspheric Coefficient 
               
             
          
           
               
                   
                 Surface # 
               
             
          
           
               
                   
                 1 
                 2 
                 4 
                 5 
                 6 
                 7 
               
               
                   
                   
               
             
          
           
               
                 K = 
                 −4.99211E+00 
                   0.00000E+00 
                 −2.76683E+00 
                 −1.05978E−01 
                 −9.44264E+00 
                 −8.14044E−01 
               
               
                 A4 = 
                   3.17804E−02 
                 −7.49594E−02 
                 −2.79510E−01 
                 −9.48993E−02 
                 −2.36368E−02 
                 −4.33032E−02 
               
               
                 A6 = 
                 −4.44694E−02 
                 −5.63114E−02 
                   7.01204E−02 
                   1.76372E−01 
                   7.28042E−03 
                   6.95890E−03 
               
               
                 A8 = 
                 −7.22686E−03 
                 −9.94422E−03 
                   7.04308E−01 
                   4.23241E−02 
                 −7.39719E−04 
                 −1.46641E−03 
               
               
                 A10 = 
                 −2.34074E−02 
                   3.23528E−02 
                 −7.13427E−01 
                 −4.83725E−02 
                 — 
                   2.69776E−04 
               
               
                 A12 = 
                 — 
                 — 
                 — 
                 — 
                 — 
                 −2.21278E−05 
               
               
                   
               
             
          
         
       
     
         [0076]    Referring to  FIG. 3 , which shows an optical lens system for taking image in accordance with a second embodiment of the present invention, and  FIG. 4  shows the aberration curve of the second embodiment of the present invention. The second embodiment of the present invention is an optical lens system for taking image comprising three lens elements with refractive power, and the optical lens system for taking image comprises: from the object side to the image side: 
         [0077]    A plastic first lens element  10  with positive refractive power has a convex object-side surface  11  and a convex image-side surface  12 , and the object-side surface  11  and the image-side surface  12  of the first lens element  10  are aspheric. 
         [0078]    A plastic second lens element  20  with negative refractive power has a concave object-side surface  21  and a convex image-side surface  22 , and the object-side surface  21  and the image-side surface  22  of the second lens element  20  are aspheric. 
         [0079]    A plastic third lens element  30  with positive refractive power has a convex object-side surface  31  and a concave image-side surface  32 , the object-side surface  31  and the image-side surface  32  of the third lens element  30  are aspheric, and each of the two surfaces is formed with an inflection point. 
         [0080]    An aperture stop  40  is located between the first lens element  10  and the second lens element  20 . 
         [0081]    An IR cut filter  50  is located behind the third lens element  30  and has no influence on the focal length of the optical lens system. 
         [0082]    A sensor cover glass  60  is located behind the IR cut filter  50  and has no influence on the focal length of the optical lens system. 
         [0083]    An image plane  70  is located behind the sensor cover glass  60 . 
         [0084]    The equation of the curve of the aspheric surfaces of the second embodiment is the same as that of the first embodiment. 
         [0085]    In the second embodiment of the optical lens system for taking image, the Abbe number of the second lens element is V2, and it satisfies the relation: V2=23.4. 
         [0086]    In the second embodiment of the optical lens system for taking image, the refractive index of the first lens element is N1, and the refractive index of the second lens element is N2, and they satisfy the relations: N1=1.543, N2=1.632. 
         [0087]    In the second embodiment of the optical lens system for taking image, the radius of curvature of the object-side surface of the first lens element is R1, the radius of curvature of the image-side surface of the first lens element is R2, the radius of curvature of the object-side surface of the second lens element is R3, the radius of curvature of the image-side surface of the second lens element is R4, the radius of curvature of the object-side surface of the third lens element is R5, the radius of curvature of the image-side surface of the third lens element is R6, they satisfy the relations: |R1/R21=0.06, R3/R4=0.55, R5/R6=0.41. 
         [0088]    In the second embodiment of the optical lens system for taking image, the focal length of the first lens element is f1, the focal length of the second lens element is f2, the focal length of the third lens element is f3, the focal length of the optical lens system for taking image is f, and they satisfy the relations: f/f1=1.22, |f/f21=1.14, f/f3=0.91. 
         [0089]    In the second embodiment of the optical lens system for taking image, the center thickness of the second lens element is CT2, the distance between the second lens element and the third lens element is T23, and they satisfy the relations: CT2=0.395 mm, T23=0.380 mm. 
         [0090]    In the second embodiment of the optical lens system for taking image, the radius of curvature of the object-side surface of the first lens element is R1, the radius of curvature of the object-side surface of the second lens element is R3, the focal length of the optical lens system for taking image is f, and they satisfy the relations: R1=2.08945 mm, |R3|=0.88007 mm, R1/f=0.47, |R3/f|=0.20. 
         [0091]    In the second embodiment of the optical lens system for taking image, the length of the optical lens system is TL, the image height of the optical lens system is ImgH, and they satisfy the relation: TL/ImgH=1.97. 
         [0092]    In the second embodiment of the optical lens system for taking image, the chief ray angle of the maximal field of view is CRA, half of the maximal field of view is HFOV, and they satisfy the relation: 
         [0000]      (tan(CRA))/(tan(HFOV))=0.68. 
         [0093]    The detailed optical data the structure of the second embodiment is shown in table 3, and the aspheric surface data is shown in table 4, wherein the units of the radius of curvature, the thickness and the focal length are expressed in mm, and HFOV is half of the maximal field of view. 
         [0000]    
       
         
               
             
               
               
               
               
               
               
               
               
             
               
               
               
               
               
               
               
               
             
           
               
                 TABLE 3 
               
             
             
               
                   
               
               
                 (Embodiment 2) 
               
               
                 f(focal length) = 4.47 mm, Fno = 2.9, HFOV (half of field of view) = 33.4 deg. 
               
             
          
           
               
                   
                   
                 Curvature 
                   
                   
                   
                   
                 Focal 
               
               
                 Surface # 
                   
                 Radius 
                 Thickness 
                 Material 
                 Index 
                 Abbe # 
                 length 
               
               
                   
               
             
          
           
               
                 0 
                 Object 
                 Plano 
                 Infinity 
                   
                   
                   
                   
               
               
                 1 
                 Lens 1 
                 2.08945(ASP) 
                 0.757 
                 Plastic 
                 1.543 
                 60.3 
                 3.65 
               
               
                 2 
                   
                 −34.53540(ASP)  
                 0.021 
               
               
                 3 
                 Ape. 
                 Plano 
                 0.771 
               
               
                   
                 Stop 
               
               
                 4 
                 Lens 2 
                 −0.88007(ASP)  
                 0.395 
                 Plastic 
                 1.632 
                 23.4 
                 −3.89 
               
               
                 5 
                   
                 −1.60798(ASP)  
                 0.380 
               
               
                 6 
                 Lens 3 
                 1.75214(ASP) 
                 1.082 
                 Plastic 
                 1.53 
                 55.8 
                 4.88 
               
               
                 7 
                   
                 4.27770(ASP) 
                 0.200 
               
               
                 8 
                 IR-filter 
                 Plano 
                 0.300 
                 Glass 
                 1.517 
                 64.1 
                 — 
               
               
                 9 
                   
                 Plano 
                 0.500 
               
               
                 10 
                 Cover 
                 Plano 
                 0.500 
                 Glass 
                 1.517 
                 64.1 
                 — 
               
               
                   
                 Glass 
               
               
                 11 
                   
                 Plano 
                 0.914 
               
               
                 12 
                 Image 
                 Plano 
               
               
                   
               
             
          
         
       
     
         [0000]    
       
         
               
             
               
               
             
               
               
               
               
               
               
               
             
               
               
               
               
               
               
               
             
           
               
                 TABLE 4 
               
             
             
               
                   
               
               
                 Aspheric Coefficient 
               
             
          
           
               
                   
                 Surface # 
               
             
          
           
               
                   
                 1 
                 2 
                 4 
                 5 
                 6 
                 7 
               
               
                   
                   
               
             
          
           
               
                 K = 
                 −3.46872E+00 
                   0.00000E+00 
                 −2.36639E+00 
                 −1.05307E−01 
                 −9.91997E+00 
                 −5.85911E−02 
               
               
                 A4 = 
                   2.91905E−02 
                 −6.94872E−02 
                 −2.59205E−01 
                 −9.30243E−02 
                 −2.55918E−02 
                 −4.85171E−02 
               
               
                 A6 = 
                 −3.52623E−02 
                 −4.10585E−02 
                   1.01750E−01 
                   1.60113E−01 
                   8.16120E−03 
                   7.44587E−03 
               
               
                 A8 = 
                   9.23385E−03 
                 −1.24565E−02 
                   4.91187E−01 
                   7.22121E−02 
                 −8.48420E−04 
                 −1.36414E−03 
               
               
                 A10 = 
                 −2.46233E−02 
                   1.96607E−02 
                 −4.48435E−01 
                 −5.50844E−02 
                 — 
                   2.47186E−04 
               
               
                 A12 = 
                 — 
                 — 
                 — 
                 — 
                 — 
                 −2.18865E−05 
               
               
                   
               
             
          
         
       
     
         [0000]    
       
         
               
               
               
             
               
               
               
               
             
           
               
                   
                 TABLE 5 
               
               
                   
                   
               
               
                   
                 Embodiment 1 
                 Embodiment 2 
               
               
                   
                   
               
             
             
               
                   
               
             
          
           
               
                   
                 f 
                 4.46 
                 4.47 
               
               
                   
                 Fno 
                 3.20 
                 2.90 
               
               
                   
                 HFOV 
                 33.4 
                 33.4 
               
               
                   
                 V2 
                 30.2 
                 23.4 
               
               
                   
                 N1 
                 1.543 
                 1.543 
               
               
                   
                 N2 
                 1.583 
                 1.632 
               
               
                   
                 f/f1 
                 1.27 
                 1.22 
               
               
                   
                 |f/f2| 
                 1.34 
                 1.14 
               
               
                   
                 f/f3 
                 1.02 
                 0.91 
               
               
                   
                 |R1/R2| 
                 0.16 
                 0.06 
               
               
                   
                 R3/R4 
                 0.47 
                 0.55 
               
               
                   
                 R5/R6 
                 0.35 
                 0.41 
               
               
                   
                 R1 
                 2.17692 
                 2.08945 
               
               
                   
                 |R3| 
                 0.86293 
                 0.88007 
               
               
                   
                 R1/f 
                 0.49 
                 0.47 
               
               
                   
                 |R3/f| 
                 0.19 
                 0.20 
               
               
                   
                 CT2 
                 0.412 
                 0.395 
               
               
                   
                 T23 
                 0.372 
                 0.380 
               
               
                   
                 tan(CRA)/tan(HFOV) 
                 0.62 
                 0.68 
               
               
                   
                 TL/ImgH 
                 1.98 
                 1.97 
               
               
                   
                   
               
             
          
         
       
     
         [0094]    It is to be noted that the tables 1-4 show different data of the different embodiments, however, the data of the different embodiments is obtained from experiments. Therefore, any product of the same structure is contemplated to be within the scope of the present invention even if it uses different data. Table 5 is the data relevant to the present invention of the respective embodiments. 
         [0095]    While we have shown and described various embodiments in accordance with the present invention, it is clear to those skilled in the art that further embodiments may be made without departing from the scope of the present invention.