Abstract:
A compact two-group zoom lens that corrects aberrations in the visible and the near-infrared regions and that provides a comparatively high aperture ratio includes, in order from the object side, a first lens group of negative refractive power and a second lens group of positive refractive power. Both lens groups include three lens components and four lens elements. The first lens group includes, in order from the object side, lens elements having negative, negative, negative, and positive refractive powers, respectively. The second lens group includes, in order from the object side, lens elements having positive, positive, negative, and positive refractive powers, respectively. Aspheric surfaces are disclosed. Certain conditions relating to the focal lengths of the two lens groups, and the index of refraction and Abbe number of one lens element are satisfied to control aberrations in both the visible and the near-infrared regions.

Description:
Lens systems for use in surveillance cameras, such as closed circuit television cameras (CCTV), both during the day and at night have been desired. Usually, an image is obtained using visible light during the day and near-infrared light at night. Therefore, lens systems with good image performance in both the visible light region and the near-infrared region are necessary. 
   In common lens systems designed for the visible light region, aberrations, particularly chromatic aberrations generated in the near-infrared region, cause the focus to undesirably shift during imaging at night. In order to avoid this undesirable focus shift, chromatic aberrations must be favorably corrected, especially in the near-infrared region and the visible light region for lens systems used in surveillance cameras. 
   Japanese Laid-Open Patent Application 2002-207166 describes a conventional zoom lens for correcting chromatic aberrations in the visible light region and in the near-infrared region. The zoom lens described in Japanese Laid-Open Patent Application 2002-207166 is a two-group zoom lens that includes an object-side lens group having negative refractive power and an image-side lens group having positive refractive power. The object-side lens group includes two lens components and three lens elements and the image-side lens group includes five lens components and six lens elements. 
   Along with chromatic aberrations being favorably corrected in both the visible light region and the near-infrared region, there is a demand for surveillance camera lens systems that provide a bright image even at low light levels through use of a large aperture ratio, as well as miniaturization of the lens system. Accordingly, development of such lens systems is desired. 
   BRIEF SUMMARY OF THE INVENTION 
   The present invention relates to a compact zoom lens that favorably corrects aberrations in both the visible light region and the near-infrared region and provides comparatively bright imaging with a relatively large aperture ratio. Additionally, the present invention relates to such a compact zoom lens that is particularly suitable for surveillance imaging in both the visible light region and the near-infrared region. 

   
     BRIEF DESCRIPTION OF THE DRAWINGS 
     The present invention will become more fully understood from the detailed description given below and the accompanying drawings, which are given by way of illustration only and thus are not limitative of the present invention, wherein: 
       FIG. 1  shows a cross-sectional view of Embodiment 1 of the zoom lens of the present invention at the wide-angle end; 
       FIGS. 2A–2C  show aberrations of Embodiment 1 of the zoom lens of the present invention at the wide-angle end; 
       FIGS. 3A–3C  show aberrations of Embodiment 1 of the zoom lens of the present invention at the telephoto end; 
       FIGS. 4A–4C  show aberrations of Embodiment 2 of the zoom lens of the present invention at the wide-angle end; and 
       FIGS. 5A–5C  show aberrations of Embodiment 2 of the zoom lens of the present invention at the telephoto end. 
   

   DETAILED DESCRIPTION 
   A general description of the two-group zoom lens of the present invention that pertains to both embodiments of the invention will first be described with reference to  FIG. 1  that shows Embodiment 1. In  FIG. 1 , lens elements are referenced by the letter L followed by a number denoting their order from the object side of the zoom lens along the optical axis Z 1 , from L 11  to L 14  and from L 21  to L 24 . Similarly, radii of curvature of the surfaces of the various optical elements, including the lens surfaces, are referenced by the letter R followed by a number denoting their order from the object side of the zoom lens, from R 1  to R 17 . The on-axis surface spacings along the optical axis Z 1  of the various optical surfaces are referenced by the letter D followed by a number denoting their order from the object side of the zoom lens, from D 1  to D 16 . In the same manner, the two lens groups are labeled G 1  and G 2  in order from the object side of the zoom lens and the lens components belonging to each lens group are indicated by the brackets adjacent the labels G 1  and G 2 . 
   The term “lens group” is defined in terms of “lens elements” and “lens components” as explained herein. The term “lens element” is herein defined as a single transparent mass of refractive material having two opposed refracting surfaces, which surfaces are positioned at least generally transversely of the optical axis of the zoom lens. The term “lens component” is herein defined as (a) a single lens element spaced so far from any adjacent lens element that the spacing cannot be neglected in computing the optical image forming properties of the lens elements or (b) two or more lens elements that have their adjacent lens surfaces either in full overall contact or overall so close together that the spacings between adjacent lens surfaces of the different lens elements are so small that the spacings can be neglected in computing the optical image forming properties of the two or more lens elements. Thus, some lens elements may also be lens components. Therefore, the terms “lens element” and “lens component” should not be taken as mutually exclusive terms. In fact, the terms may frequently be used to describe a single lens element in accordance with part (a) above of the definition of a “lens component.” The term “lens group” is herein defined as an assembly of one or more lens components in optical series and with no intervening lens components along an optical axis that during zooming is movable as a single unit relative to another lens component or other lens components. 
   As shown in  FIG. 1 , a diaphragm stop St that controls the amount of light that passes through the zoom lens is included between the lens groups G 1  and G 2 . Also as shown in  FIG. 1 , a cover glass GC is arranged on the image side of the second lens group G 2 . 
   The zoom lens is designed for use in both the visible light region and the near-infrared region and is particularly suited for mounting in a surveillance camera for use both during the day and at night. As shown in  FIG. 1 , the two-group zoom lens of the present invention includes, in order from the object side, a first lens group G 1  having negative refractive power and a second lens group G 2  having positive refractive power. 
   An image pickup element (not shown in the drawings), such as a CCD (Charge-Coupled Device) or CMOS (Complementary Metal-Oxide Semiconductor), is arranged at an image plane (not shown in the drawings) on the image side of the cover glass GC. Various other optical elements may also be arranged between the second lens group G 2  and the image plane. 
   The two-group zoom lens zooms from the wide-angle end to the telephoto end by moving the second lens group G 2  toward the object side along the optical axis Z 1  in order to change the focal length of the zoom lens, and compensates for movement of the image plane caused by movement of the second lens group G 2  by moving the first lens group G 1  toward the image side during zooming from the wide-angle end to the telephoto end of the zoom range. Downward arrows at the bottom of  FIG. 1  show the directions of movement along the optical axis Z 1  of the first lens group G 1  and the second lens group G 2  when zooming from the wide-angle end to the telephoto end, as indicated by the symbols “WIDE” and “TELE”, respectively, in  FIG. 1 . The first lens group G 1  also functions as a focusing lens group. 
   Preferably, the zoom lens satisfies the following condition:
 
0.5 &lt;|f 1 /f 2 |&lt;0.8  Condition (1)
 
where
 
   f 1  is the focal length of the first lens group G 1 , and 
   f 2  is the focal length of the second lens group G 2 . 
   Aberrations are readily corrected and the zoom lens may be kept compact by satisfying Condition (1). If the value of Condition (1) does not satisfy the upper limit of Condition (1), the refractive power of the first lens group G 1  becomes too weak and the first lens group must be moved too far during zooming so that compactness of the zoom lens cannot be maintained. If the value of Condition (1) does not satisfy the lower limit of Condition (1), the refractive power of the first lens group becomes too strong and sufficient correction of spherical aberration at the telephoto end cannot be achieved. 
   The first lens group G 1  includes three lens components and four lens elements, in order from the object side, as follows: a first lens element L 11  having negative refractive power; a second lens element L 12  having negative refractive power; and a lens component that includes, in order from the object side, a third lens element L 13  having negative refractive power that is intimately bonded to a fourth lens element L 14  having positive refractive power. The term “intimately bonded” is defined herein generally to mean that adjacent refractive surfaces of two lens elements have substantially the same curvature and are held in direct fixed contact or are separated by a thin layer of transparent adhesive (too thin to be considered in optical computations) that fixes the lenses together, the latter being commonly referred to as a “cemented” lens element arrangement. 
   In the first lens group G 1 , the first lens element L 11  and the second lens element L 12  are meniscus lens elements with the convex surface on the object side, the third lens element L 13  is a biconcave lens element, and the fourth lens element L 14  is a meniscus lens element with the convex surface on the object side. 
   The second lens group G 2  includes, in order from the object side, a first lens element L 21  having positive refractive power, a lens component that includes, in order from the object side, a second lens element L 22  having positive refractive power that is intimately bonded to a third lens element L 23  having negative refractive power, and a fourth lens element L 24  having positive refractive power, arranged on the image side of the zoom lens, and having at least one aspheric surface. 
   In the second lens group G 2 , the first lens element L 21  is a meniscus lens element with the convex surface on the object side, the second lens element L 22  is a biconvex lens element, and the third lens element L 23  is a biconcave lens element. The fourth lens element L 24  has a biconvex shape near the optical axis. When the surface on the object side of the fourth lens element L 24  is made to be aspheric, it is preferable that the surface on the object side have a shape so that the positive refractive power becomes weaker toward the periphery of the lens element. 
   Preferably, the second lens element L 22  of the second lens group G 2  satisfies the following conditions:
 
 N   d22 &lt;1.55  Condition (2)
 
 v   d22 &gt;65  Condition (3)
 
where
 
   N d22  is the index of refraction at the d-line (587.6 nm) of the second lens element L 22  of the second lens group G 2 , and 
   v d22  is the Abbe number at the d-line (587.6 nm) of the second lens element L 22  of the second lens group G 2 . 
   With this zoom lens, the generation of axial chromatic aberration is especially restrained by using the two-element lens components of the first lens group G 1  and the second lens group G 2 . Conditions (2) and (3) above prescribe the appropriate kind of glass for the second lens element L 22  of the second lens group G 2 . Additionally, axial chromatic aberration can be favorably corrected in both the visible light region and the near-infrared region by properly selecting the kind of glass so as to satisfy Conditions (2) and (3) so that a zoom lens with high optical performance in both these regions can be obtained. 
   In order to improve imaging, at least some of the lens surfaces of the two-group zoom lens are aspheric lens surfaces. All the aspheric lens surfaces of the zoom lens are defined using the following equation:
 
 Z =[( C·Y   2 )/{1+(1 −K·C   2   ·Y   2 ) 1/2 }]+Σ( A   i   ·Y   i )  Equation ( A )
 
where
         Z is the length (in mm) 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,   C is the curvature (=1/the radius of curvature, R) of the aspheric lens surface on the optical axis,   Y is the distance (in mm) from the optical axis,   K is the eccentricity, and   A i  is the ith aspheric coefficient, and the summation extends over i equals three to ten.       

   In embodiments of the invention disclosed below, only aspheric coefficients A 3 –A 10  are non-zero. 
   With the zoom lens of the present invention, the correction of aberrations, especially the correction of spherical aberration and lateral color at the telephoto end, are achieved more easily while achieving sufficient compactness by the first lens group G 1  having a three component, four element construction, as compared to a two component, three element construction. Additionally, compactness and a large aperture ratio are readily achieved by providing the fourth lens element L 24  of the second lens group G 2 , which lens element has positive refractive power, with an aspheric surface on the image side, thus providing an aspheric surface on the image-side lens surface of the second lens group G 2 . 
   Thus, the zoom lens of the present invention enables a small size and large aperture ratio while obtaining an optical performance suitable for a surveillance camera that operates in both the visible light region and the near-infrared region with more detailed construction determined by the particular demands of use. For example, the zoom lens may be designed so that no focus adjustment is needed when ambient light conditions change from bright to low light levels or when ambient light conditions change from visible light to near-infrared. 
   Embodiments 1 and 2 of the present invention will now be individually described with further reference to the drawings. 
   EMBODIMENT 1 
   Table 1 below lists the surface number #, in order from the object side, the radius of curvature R (in mm) of each surface near the optical axis, the on-axis surface spacing D (in mm), as well as the refractive index N d  and the Abbe number v d  (both at the d-line of 587.6 nm) of each optical element for Embodiment 1. 
   
     
       
             
             
             
             
             
           
         
             
               TABLE 1 
             
             
                 
             
             
               # 
               R 
               D 
               N d   
               ν d   
             
             
                 
             
           
           
             
                1 
               35.912 
               0.750 
               1.69680 
               55.5 
             
             
                2 
               7.724 
               0.500 
             
             
                3 
               9.596 
               0.800 
               1.69895 
               30.1 
             
             
                4 
               5.536 
               3.557 
             
             
                5 
               −10.500 
               0.640 
               1.49700 
               81.6 
             
             
                6 
               9.821 
               2.580 
               1.84666 
               23.8 
             
             
                7 
               64.005 
                D7 (variable) 
             
             
                8 
               ∞ (stop) 
                D8 (variable) 
             
             
                9 
               10.978 
               2.899 
               1.72916 
               54.7 
             
             
               10 
               74.972 
               0.485 
             
             
               11 
               8.228 
               4.609 
               1.49700 (N d22 ) 
               81.6 (ν d22 ) 
             
             
               12 
               −17.962 
               0.650 
               1.84666 
               23.8 
             
             
               13 
               9.189 
               0.258 
             
             
                14* 
               7.274 
               4.356 
               1.69350 
               53.2 
             
             
                15* 
               −11.868 
               D15 (variable) 
             
             
               16 
               ∞ 
               3.320 
               1.51633 
               64.1 
             
             
               17 
               ∞ 
             
             
                 
             
             
               The surfaces with a * to the right of the surface number in Table 1 are aspheric lens surfaces, and the aspheric surface shape is expressed by Equation (A) above. As indicated in Table 1, both surfaces of the fourth lens element L24 of the second lens group G2 are aspheric. 
             
           
        
       
     
   
   Table 2 below lists the values of the constants K, and A 3 –A 10  used in Equation (A) above for each of the aspheric lens surfaces of Table 1. Aspheric coefficients that are not present in Table 2 are zero. An “E” in the data indicates that the number following the “E” is the exponent to the base  10 . For example, “1.0E−2” represents the number 1.0×10 −2 . 
   
     
       
             
             
             
             
             
             
           
             
             
             
             
             
           
         
             
               TABLE 2 
             
             
                 
             
           
           
             
               # 
               K 
               A 3   
               A 4   
               A 5   
               A 6   
             
             
                 
             
             
               14 
               −0.3119479 
               −0.1218642E−2 
                 0.7246816E−3 
               −0.6302984E−3 
                 0.7570227E−4 
             
             
               15 
               −2.2183366 
               −0.1553495E−2 
                 0.1292285E−2 
               −0.5186717E−3 
                 0.3768057E−4 
             
             
                 
             
           
        
         
             
               # 
               A 7   
               A 8   
               A 9   
               A 10   
             
             
                 
             
             
               14 
                 0.1189115E−4 
               −0.3574370E−5 
               −0.2590567E−6 
                 0.5284200E−7 
             
             
               15 
                 0.3353471E−5 
                 0.1270727E−6 
               −0.1234525E−6 
               −0.1419697E−7 
             
             
                 
             
           
        
       
     
   
   In the zoom lens of Embodiment 1, both the first lens group G 1  and the second lens group G 2  move during zooming. Therefore, the on-axis spacings D 7 , D 8 , and D 15  change with zooming. With zooming, the focal length f, the f-number F NO , and the field angle  2 ω of the zoom lens also change. Table 3 below lists the values of the focal length f (in mm), the f-number F NO , the field angle  2 ω (in degrees), and the variables D 7 , D 8 , and D 15  (in mm) at the wide-angle end (f=2.49 mm) and the telephoto end (f=5.68 mm) when the zoom lens is focused at infinity. 
   
     
       
             
             
             
             
             
             
             
           
             
             
             
             
             
             
             
           
         
             
                 
               TABLE 3 
             
             
                 
                 
             
             
                 
               f 
               F NO   
               2ω 
               D7 
               D8 
               D15 
             
             
                 
                 
             
           
           
             
                 
             
           
        
         
             
                 
               2.49 
               0.95 
               114 
               9.93 
               5.48 
               2.00 
             
             
                 
               5.68 
               1.53 
               46 
               2.10 
               0.88 
               6.60 
             
             
                 
                 
             
           
        
       
     
   
   The zoom lens of Embodiment 1 of the present invention satisfies Conditions (1)–(3) above as set forth in Table 4 below. 
   
     
       
             
             
             
           
             
             
             
           
         
             
               TABLE 4 
             
             
                 
             
             
               Condition No. 
               Condition 
               Value 
             
             
                 
             
           
           
             
                 
             
           
        
         
             
               (1) 
               0.5 &lt; |f1/f2| &lt; 0.8 
               0.69 
             
             
               (2) 
               N d22  &lt; 1.55 
               1.49700 
             
             
               (3) 
               ν d22  &gt; 65 
               81.6 
             
             
                 
             
           
        
       
     
   
     FIGS. 2A–2C  show the spherical aberration, astigmatism, and distortion, respectively, of the zoom lens of Embodiment 1 at the wide-angle end.  FIGS. 3A–3C  show the spherical aberration, astigmatism, and distortion, respectively, of the zoom lens of Embodiment 1 at the telephoto end. In  FIGS. 2A and 3A , the spherical aberration is shown for the wavelengths 587.6 nm (the d-line) and 880 nm. In  FIGS. 2B ,  2 C,  3 B, and  3 C, ω is the half-field angle. In  FIGS. 2B and 3B , the astigmatism is shown for the sagittal image surface S and the tangential image surface T. In  FIGS. 2C and 3C , distortion is measured at 587.6 nm (the d-line). As is apparent from these figures, the various aberrations are favorably corrected over the entire range of zoom and in both the visible light and near-infrared regions with the compact zoom lens with a relatively large aperture ratio of Embodiment 1. 
   EMBODIMENT 2 
   Embodiment 2 is very similar to Embodiment 1 and therefore only the differences between Embodiment 2 and Embodiment 1 will be explained. Embodiment 2 differs from Embodiment 1 in its lens element configuration such as some different radii of curvature of the lens surfaces, different eccentricities and aspheric coefficients of the aspheric lens surfaces, some different optical element surface spacings, some different refractive indexes, and some different Abbe numbers of the optical materials of the lens elements. 
   Table 5 below lists the surface number #, in order from the object side, the radius of curvature R (in mm) of each surface near the optical axis, the on-axis surface spacing D (in mm), as well as the refractive index N d  and the Abbe number V d  (both at the d-line of 587.6 nm) of each optical element for Embodiment 2. 
   
     
       
             
             
             
             
             
           
         
             
               TABLE 5 
             
             
                 
             
             
               # 
               R 
               D 
               N d   
               ν d   
             
             
                 
             
           
           
             
                1 
               27.798 
               0.750 
               1.75500 
               52.3 
             
             
                2 
               7.962 
               0.500 
             
             
                3 
               9.615 
               0.800 
               1.75520 
               27.5 
             
             
                4 
               5.550 
               3.557 
             
             
                5 
               −10.500 
               0.640 
               1.49700 
               81.6 
             
             
                6 
               9.821 
               2.580 
               1.84666 
               23.8 
             
             
                7 
               64.005 
                D7 (variable) 
             
             
                8 
               ∞ (stop) 
                D8 (variable) 
             
             
                9 
               11.047 
               2.882 
               1.69680 
               55.5 
             
             
               10 
               74.985 
               0.438 
             
             
               11 
               7.821 
               4.739 
               1.49700 (N d22 ) 
               81.6 (ν d22 ) 
             
             
               12 
               −19.779 
               0.650 
               1.84666 
               23.8 
             
             
               13 
               8.808 
               0.301 
             
             
                14* 
               7.124 
               4.265 
               1.69350 
               53.2 
             
             
                15* 
               −11.945 
               D15 (variable) 
             
             
               16 
               ∞ 
               3.320 
               1.51633 
               64.1 
             
             
               17 
               ∞ 
             
             
                 
             
             
               The surfaces with a * to the right of the surface number in Table 5 are aspheric lens surfaces, and the aspheric surface shape is expressed by Equation (A) above. As indicated in Table 5, both surfaces of the fourth lens element L24 of the second lens group G2 are aspheric. 
             
           
        
       
     
   
   Table 6 below lists the values of the constants K, and A 3 –A 10  used in Equation (A) above for each of the aspheric lens surfaces of Table 5. Aspheric coefficients that are not present in Table 6 are zero. An “E” in the data indicates that the number following the “E” is the exponent to the base  10 . For example, “1.0E−2” represents the number 1.0×10 −2 . 
   
     
       
             
             
             
             
             
             
           
             
             
             
             
             
           
         
             
               TABLE 6 
             
             
                 
             
           
           
             
               # 
               K 
               A 3   
               A 4   
               A 5   
               A 6   
             
             
                 
             
             
               14 
               −0.4878057 
               −0.9808512E−3 
                 0.3104345E−3 
               −0.3942310E−3 
                 0.2909605E−4 
             
             
               15 
               −2.4098731 
               −0.1634326E−2 
                 0.1315548E−2 
               −0.5586721E−3 
                 0.4228572E−4 
             
             
                 
             
           
        
         
             
               # 
               A 7   
               A 8   
               A 9   
               A 10   
             
             
                 
             
             
               14 
                 0.1191683E−4 
               −0.3296691E−5 
               −0.2360361E−6 
                 0.5284274E−7 
             
             
               15 
                 0.3792502E−5 
                 0.3222287E−7 
               −0.1321672E−6 
               −0.1398418E−7 
             
             
                 
             
           
        
       
     
   
   In the zoom lens of Embodiment 2, both the first lens group G 1  and the second lens group G 2  move during zooming. Therefore, the on-axis spacings D 7 , D 8 , and D 15  change with zooming. With zooming, the focal length f, the f-number F NO , and the field angle  2 ω of the zoom lens also change. Table 7 below lists the values of the focal length f (in mm), the f-number F NO , the field angle  2 ω (in degrees), and the variables D 7 , D 8 , and D 15  (in mm) at the wide-angle end (f=2.49 mm) and the telephoto end (f=5.69 mm) when the zoom lens is focused at infinity. 
   
     
       
             
             
             
             
             
             
             
           
             
             
             
             
             
             
             
           
         
             
                 
               TABLE 7 
             
             
                 
                 
             
             
                 
               f 
               F NO   
               2ω 
               D7 
               D8 
               D15 
             
             
                 
                 
             
           
           
             
                 
             
           
        
         
             
                 
               2.49 
               0.95 
               112 
               9.93 
               5.46 
               2.00 
             
             
                 
               5.69 
               1.53 
               46 
               2.11 
               0.85 
               6.61 
             
             
                 
                 
             
           
        
       
     
   
   The zoom lens of Embodiment 2 of the present invention satisfies Conditions (1)–(3) above as set forth in Table 8 below. 
   
     
       
             
             
             
           
             
             
             
           
         
             
               TABLE 8 
             
             
                 
             
             
               Condition No. 
               Condition 
               Value 
             
             
                 
             
           
           
             
                 
             
           
        
         
             
               (1) 
               0.5 &lt; |f1/f2| &lt; 0.8 
               0.69 
             
             
               (2) 
               N d22  &lt; 1.55 
               1.49700 
             
             
               (3) 
               ν d22  &gt; 65 
               81.6 
             
             
                 
             
           
        
       
     
   
     FIGS. 4A–4C  show the spherical aberration, astigmatism, and distortion, respectively, of the zoom lens of Embodiment 2 at the wide-angle end.  FIGS. 5A–5C  show the spherical aberration, astigmatism, and distortion, respectively, of the zoom lens of Embodiment 2 at the telephoto end. In  FIGS. 4A and 5A , the spherical aberration is shown for the wavelengths 587.6 nm (the d-line) and 880 nm. In  FIGS. 4B ,  4 C,  5 B, and  5 C, ω is the half-field angle. In  FIGS. 4B and 5B , the astigmatism is shown for the sagittal image surface S and the tangential image surface T. In  FIGS. 4C and 5C , distortion is measured at 587.6 nm (the d-line). As is apparent from these figures, the various aberrations are favorably corrected over the entire range of zoom and in both the visible light and near-infrared regions with the compact zoom lens with a relatively large aperture ratio of Embodiment 2. 
   The present invention is not limited to the aforementioned embodiments, as it will be obvious that various alternative implementations are possible. For instance, values such as the radius of curvature R of each of the lens components, the surface spacings D, the refractive index N, as well as the Abbe number v, are not limited to the examples indicated in each of the aforementioned embodiments, as other values can be adopted. Such variations are not to be regarded as a departure from the spirit and scope of the present invention. Rather, the scope of the present invention shall be defined as set forth in the following claims and their legal equivalents. All such modifications as would be obvious to one skilled in the art are intended to be included within the scope of the following claims.