# Patent

## Title
Camera lens

## Abstract

A camera lens is disclosed and includes from the object side to the image side: a first lens with positive refractive power; a second lens with negative refractive power; a third lens with negative refractive power; a fourth lens with positive refractive power; a fifth lens with positive refractive power; and a sixth lens with negative refractive power. Specific conditions are satisfied.

## Background
FIELD OF THE INVENTION
The present invention relates to a camera lens, particularly relates to a camera lens in which high-pixel CCD, CMOS camera elements are used, such as the mobile phone camera module, WEB camera etc.
DESCRIPTION OF RELATED ART
In recent years, a variety of cameras equipped with CCD, CMOS and other camera elements are extensively popular. Along with the development of miniature and high performance camera elements, the ultrathin and high-luminous flux F (Fno) wide-angle camera lenses with excellent optical properties are needed in society.
The technology related to the camera lens composed of six ultra-thin, high-luminous flux f value (Fno) wide angle lenses with excellent optical properties is developed gradually. The camera lens mentioned in the proposal is composed of 6 lenses, lined up from the object side in an order as follows: The first lens with positive refractive power; the second lens with negative refractive power; the third lens with negative refractive power; the fourth lens with positive refractive power; the fifth lens with positive refractive power and the sixth lens with negative refractive power.
The camera lens disclosed in a related reference is composed of 6 lenses, but the refractive index power of the first lens and the third lens is inadequate; the shape of the second lens is improper; the proportion of the axial distance between the image side of the forth lens and the object side of the sixth lens to the overall focus distance of the camera lens is not proper, therefore, 2ω=75.8°, Fno=2.4, wide-angle and Fno luminous flux are not sufficient.
The camera lens disclosed in another related reference is composed of 6 lenses, but the refractive index power of the first lens and the third lens is inadequate; the shape of the second lens is improper, therefore, 2ω≦77.0°, TTL/IH≧1.464, wide angle and ultrathin degree is not sufficient.
The present invention provides an improved camera lens to solve the problems.



BRIEF DESCRIPTION OF THE DRAWINGS
Many aspects of the embodiments can be better understood with reference to the following drawings. The components in the drawings are not necessarily drawn to scale, the emphasis instead being placed upon clearly illustrating the principles of the present disclosure. Moreover, in the drawings, like reference numerals designate corresponding parts throughout the several views.
FIG. 1 is a structural diagram of a camera lens LA in one embodiment of the present invention;
FIG. 2 is a structural diagram of a camera lens of embodiment 1 of the disclosure;
FIG. 3 is a diagram of the spherical aberration (axial chromatic aberration) of the camera lens LA in embodiment 1;
FIG. 4 is a diagram of the magnification chromatic aberration of the camera lens LA in embodiment 1;
FIG. 5 is a diagram of the image side curving and distortion aberration of the camera lens LA in embodiment 1;
FIG. 6 is a structural diagram of a camera lens of embodiment 2 of the disclosure;
FIG. 7 is a diagram of the spherical aberration (axial chromatic aberration) of the camera lens LA in embodiment 2;
FIG. 8 is a diagram of the magnification chromatic aberration of the camera lens LA in embodiment 2;
FIG. 9 is a diagram of the image side curving and distortion aberration of the camera lens LA in embodiment 2;
FIG. 10 is a structural diagram of a camera lens of embodiment 3 of the disclosure;
FIG. 11 is a diagram of the spherical aberration (axial chromatic aberration) of the camera lens LA in embodiment 3;
FIG. 12 is a diagram of the magnification chromatic aberration of the camera lens LA in embodiment 3;
FIG. 13 is a diagram of the image side curving and distortion aberration of the camera lens LA in embodiment 3



DESCRIPTION OF REFERENCE NUMBERS OR LABELS
The reference numbers or labels in all embodiments are represented as follows, in which, the unit of the distance, radius and center thickness is mm.

    LA: Camera lens
    S1: Open aperture
    L1: The first lens
    L2: The second lens
    L3: The third lens
    L4: The fourth lens
    L5: The fifth lens
    L6: The sixth lens
    GF: Glass plate
    f: Overall focal distance of the camera lens LA
    f1: The focal distance of the first lens L1
    f2: The focal distance of the second lens L2
    f3: The focal distance of the third lens L3
    f4: The focal distance of the fourth lens L4
    f5: The focal distance of the fifth lens L5
    f6: The focal distance of the sixth lens L6
    Fno: F value
    2ω: Total angle of view
    R: Curvature radius of image side is the center curvature radius of the lens.
    R1: The object side curvature radius of the first lens L1
    R2: The image side curvature radius of the first lens L1
    R3: The object side curvature radius of the second lens L2
    R4: The image side curvature radius of the second lens L2
    R5: The object side curvature radius of the third lens L3
    R6: The image side curvature radius of the third lens L3
    R7: The object side curvature radius of the fourth lens L4
    R8: The image side curvature radius of the fourth lens L4
    R9: The object side curvature radius of the fifth lens L5
    R10: The image side curvature radius of the fifth lens L5
    R11: The object side curvature radius of the sixth lens L6
    R12: The image side curvature radius of the sixth lens L6
    R13: The object side curvature radius of the glass plate GF
    R14: The image side curvature radius of glass plate GF
    d: The center thickness of lenses and the distance between lenses
    d1: The center thickness of the first lens L1
    d2: The distance from the image side to the aperture S1 of the first lens L1
    d3: The axial distance from the open aperture S1 to the object side of second lens L2
    d4: The center thickness of the second lens L2
    d5: The axial distance between the image side of the second lens L2 and the object side of the third lens L3
    d6: The center thickness of the third lens L3
    d7: The axial distance between the image side of the third lens L3 and the object side of the fourth lens L4
    d8: The center thickness of the fourth lens L4
    d9: The axial distance between the image side of the fourth lens L4 and the object side of the fifth lens L5
    d10: The center thickness of the fifth lens L5
    d11: The axial distance between the image side of fifths lens L5 and the object side of sixth lens L6
    d12: The center thickness of the sixth lens L6
    d13: The axial distance between the image side of the sixth lens L6 and the object side of the glass plate GF
    d14: The center thickness of the glass plate GF
    d15: The axial distance from the image side to the imaging plane of the glass plate GF
    nd: Refractive power of line d
    nd1: Refractive power of line d of the first lens L1
    nd2: Refractive power of line d of the second lens L2
    nd3: Refractive power of line d of the third lens L3
    nd4: Refractive power of line d of the fourth lens L4
    nd5: Refractive power of line d of the fifth lens L5
    nd6: Refractive power of line d of the sixth lens L6
    nd7: Refractive power of line d of glass plate GF
    v: Abbe number
    v1: Abbe number of the first lens L1
    v2: Abbe number of the second lens L2
    v3: Abbe number of the third lens L3
    v4: Abbe number of the fourth lens L4
    v5: Abbe number of the fifth lens L5
    v6: Abbe number of the sixth lens L6
    v7: Abbe number of the glass plate GF
    TTL: Optical length (the axial distance from the object side to the imaging plane of the first lens L1)
    LB: The axial distance from the image side to the imaging plane of the sixth
    lens L6 (including the thickness of the glass plate GF)
    IH: Image height


DETAILED DESCRIPTION OF THE EXEMPLARY EMBODIMENTS
The present invention will hereinafter be described in detail with reference to exemplary embodiments. To make the technical problems to be solved, technical solutions and beneficial effects of present disclosure more apparent, the present disclosure is described in further detail together with the Fig.s and the embodiments. It should be understood the specific embodiments described hereby is only to explain this disclosure, not intended to limit this disclosure.
The reference Fig.s explains one embodiment of the camera lens in the present invention. FIG. 1 shows the structural diagram of one embodiment of the camera lens of the present invention. The camera lens LA includes six lenses, which are lined up from the object side to the image side in an order as follows: a first lens L1, a second lens L2, a third lens L3, a fourth lens L4, a fifth lens L5 and a sixth lens L6. A glass plate GF is provided between the sixth lens L6 and the imaging plane. The glass plate GF is a cover glass or a light filter having IR cut-off filtration and other functions; or the glass plate GF is not be provided between the sixth lens L6 and the imaging plane.
The first lens L1 has positive refractive power; the second lens L2 has negative refractive power; the third lens L3 has negative refractive power; the fourth lens L4 has positive refractive power; the fifth lens L5 has positive refractive power and the sixth lens L6 has negative refractive power. In order to correct aberration better, the surface of six lenses is best designed to be non-spherical shape.
The camera lens LA satisfies the following condition expressions (1) to (4):

0.85≦f1/f≦1.10  (1)

−10.00≦f3/f≦−4.50  (2)

2.50≦(R3+R4)/(R3−R4)≦4.00  (3)

0.08≦d11/f≦0.15  (4)

In which:

f: The overall focal distance of the camera lens LA;

f1: The focal distance of the first lens;

f3: The focal distance of the third lens;

R3: The object side curvature radius of the second lens;

R4: The image side curvature radius of the second lens;

d11: The axial distance between the image side of the fifth lens and the object side of the sixth lens.

The condition expression (1) specifies the positive refractive power of the first lens L1. When exceeding the lower limit value of the condition expression (1), although in favor of the ultra-thin development of the lens, the first lens L1 has too big positive refractive power, it is difficult to correct the aberration and other issues. On the contrary, when exceeding the upper limit, the first lens has too small positive refractive power, not conducive to the ultrathin development of lens.
The condition expression (2) specifies the negative refractive power of the third lens L3. If exceeding the limit of the condition expression (2), along with Fno≦2.2 ultra-thin and wide-angle development of the lens, it is difficult to correct magnification chromatic aberration.
The condition expression (3) specifies the shape of the second lens L2. If exceeding the limit of the condition expression (3), along with Fno≦2.2 ultra-thin and wide-angle development of the lens, it is difficult to correct the axial chromatic aberration.
The condition expression (4) specifies the proportion of the distance between the image side of the forth lens and the object side of the sixth lens to the overall focus distance of the camera lens LA. When exceeding the lower limit of the condition expression (4), although in favor of the ultra-thin development of the lens, it is difficult to correct the abaxial chromatic aberration in corresponding view angle. When exceeding the upper limit value, it is not conducive to the ultra-thin development of the lens.
The second lens L2 has positive refractive power and satisfies the following condition expression (5):

−2.50≦f2/f≦−1.00  (5)

In which:
f: The overall focal distance of the camera lens LA;
f2: The focal distance of the second lens;
The condition expression (5) specifies the negative refractive power of the second lens L2. If exceeding the limit of the condition expression (5), along with Fno≦2.2 ultra-thin and wide-angle development of the lens, it is difficult to correct the axial chromatic aberration.
The fourth lens L4 has positive refractive power and satisfies the following condition expression (6).

2.50≦f4/f≦6.00  (6)

In which, f is the overall focal distance of the camera lens LA; f4 is the focal distance of the fourth lens.

The condition expression (6) specifies the positive refractive power of the fourth lens L4. If exceeding the limit of the condition expression (6), it is not conducive to Fno≦2.2 ultra-thin and wide-angle development of lens.
The first lens L1 has positive refractive power and satisfies the following condition expression (7).

−1.50≦(R1+R2)/(R1−R2)≦−0.50  (7)

In which, R1 is the object side curvature radius of the first lens; R2 is the image side curvature radius of the first lens.

The condition expression (7) specifies the shape of the first lens L1. If exceeding the limit of the condition expression (7), along with Fno≦2.2 ultra-thin and wide-angle development of the lens, it is difficult to correct the spherical aberration and other higher aberration issues.
The third lens L3 has negative refractive power and satisfies the following condition expression (8).

1.00≦(R5+R6)/(R5−R6)≦5.00  (8)

In which:

R5: The object side curvature radius of the third lens;

R6: The image side curvature radius of the third lens;

The condition expression (8) specifies the shape of the third lens L3. If exceeding the limit of the condition expression (8), along with Fno≦2.2 ultra-thin and wide-angle development of the lens, it is difficult to correct magnification chromatic aberration issues.
As six lenses of the camera lens LA have the structure described previously and meet all condition expressions, the camera lens composed of six TTL (optical length)/IH (image height)≦1.45, ultrathin, wide-angle 2ω≧82°, high-luminous flux Fno≦2.2 lenses with excellent optical properties can be produced.
EMBODIMENTS
The camera lens LA of the present invention is described with the embodiments as follows. The symbols in all embodiments are represented as follows. In addition, the unit of the distance, radius and center thickness is mm.
f: Overall focal distance of the camera lens LA
f1: The focal distance of the first lens L1
f2: The focal distance of the second lens L2
f3: The focal distance of the third lens L3
f4: The focal distance of the fourth lens L4
f5: The focal distance of the fifth lens L5
f6: The focal distance of the sixth lens L6
Fno: F value
2ω: Total angle of view
S1: Open aperture
R: Curvature radius of image side is the center curvature radius of the lens.
R1: The object side curvature radius of the first lens L1
R2: The image side curvature radius of the first lens L1
R3: The object side curvature radius of the second lens L2
R4: The image side curvature radius of the second lens L2
R5: The object side curvature radius of the third lens L3
R6: The image side curvature radius of the third lens L3
R7: The object side curvature radius of the fourth lens L4
R8: The image side curvature radius of the fourth lens L4
R9: The object side curvature radius of the fifth lens L5
R10: The image side curvature radius of the fifth lens L5
R11: The object side curvature radius of the sixth lens L6
R12: The image side curvature radius of the sixth lens L6
R13: The object side curvature radius of the glass plate GF
R14: The image side curvature radius of glass plate GF
d: The center thickness of lenses and the distance between lenses
d1: The center thickness of the first lens L1
d2: The distance from the image side to the aperture S1 of the first lens L1
d3: The axial distance from the open aperture S1 to the object side of second lens L2
d4: The center thickness of the second lens L2
d5: The axial distance between the image side of the second lens L2 and the object side of the third lens L3
d6: The center thickness of the third lens L3
d7: The axial distance between the image side of the third lens L3 and the object side of the fourth lens L4
d8: The center thickness of the fourth lens L4
d9: The axial distance between the image side of the fourth lens L4 and the object side of the fifth lens L5
d10: The center thickness of the fifth lens L5
d11: The axial distance between the image side of fifths lens L5 and the object side of sixth lens L6
d12: The center thickness of the sixth lens L6
d13: The axial distance between the image side of the sixth lens L6 and the object side of the glass plate GF
d14: The center thickness of the glass plate GF
d15: The axial distance from the image side to the imaging plane of the glass plate GF
nd: Refractive power of line d
nd1: Refractive power of line d of the first lens L1
nd2: Refractive power of line d of the second lens L2
nd3: Refractive power of line d of the third lens L3
nd4: Refractive power of line d of the fourth lens L4
nd5: Refractive power of line d of the fifth lens L5
nd6: Refractive power of line d of the sixth lens L6
nd7: Refractive power of line d of glass plate GF
v: Abbe number
v1: Abbe number of the first lens L1
v2: Abbe number of the second lens L2
v3: Abbe number of the third lens L3
v4: Abbe number of the fourth lens L4
v5: Abbe number of the fifth lens L5
v6: Abbe number of the sixth lens L6
v7: Abbe number of the glass plate GF
TTL: Optical length (the axial distance from the object side to the imaging plane of the first lens L1)
LB: The axial distance from the image side to the imaging plane of the sixth lens L6 (including the thickness of the glass plate GF)
IH: Image height

y=(x2/R)/[1+{1−(k+1)(x2/R2)}1⁄2]+A4×4+A6×6+A8×8+A10×10+A12×12+A14×14+A16×16   (9)

In which, R is the axial curvature radius; k is the cone constant, A4, A6, A8, A10, A12, A14, A16 are aspherical coefficients.

As a matter of convenience, the aspheric surface of all lenses adopts the aspheric surface in condition expression (9). But not limited to the polynomial forms of the aspheric surface in the condition expression (9).
Embodiment 1
FIG. 2 is the structural diagram of a camera lens LA in embodiment 1. The curvature radius R of the object side and image side of the first lens L1 to sixth lens L6, center thickness of the lenses or the distance d between the lenses, refractive power nd, Abbe number v of the camera lens LA in the embodiment 1 are shown in table 1. The cone constant k and aspherical coefficient are shown in table 2.











TABLE 1






R
d
nd
vd






















R1
2.03282
d1 =
0.558
nd1
1.5441
v1
56.12


R2
−19.93247
d2 =
0.072






S1
∞
d3 =
−0.020






R3
2.78316
d4 =
0.216
nd2
1.6422
v2
22.41


R4
1.64715
d5 =
0.270






R5
42.51913
d6 =
0.220
nd3
1.6422
v3
22.41


R6
9.27262
d7 =
0.058






R7
5.68102
d8 =
0.476
nd4
1.5441
v4
56.12


R8
52.62998
d9 =
0.436






R9
−6.99008
d10 =
0.546
nd5
1.5441
v5
56.12


R10
−1.09011
d11 =
0.477






R11
−2.93771
d12 =
0.329
nd6
1.5441
v6
56.12


R12
1.76981
d13 =
0.520






R13
∞
d14 =
0.210
nd7
1.5168
v6
64.17


R14
∞
d15 =
0.269


















TABLE 2








Cone Constant
Aspherical Coeffecient
















k
A4
A6
A8
A10
A12
A14
A16


















R1
−8.5177E−01
6.4257E−04
4.3220E−03
−8.2039E−03
−1.4208E−04
3.0955E−03
4.5870E−03
−1.1337E−02


R2
0.0000E+00
2.6822E−02
−1.6747E−02
−3.2933E−03
−1.3521E−03
−7.1245E−03
−5.6572E−02
4.3199E−02


R3
−1.3917E+01
−5.1856E−03
2.6893E−02
7.3495E−03
−2.9717E−02
−3.6417E−02
−6.1611E−02
1.0379E−01


R4
−4.5526E+00
−2.1692E−02
9.6074E−03
3.5787E−02
−4.8609E−02
−8.3232E−02
−4.4927E−02
2.0432E−01


R5
4.1544E+02
2.1863E−03
−1.0180E−01
−4.6675E−02
3.0465E−03
−2.3599E−02
−7.3970E−02
2.6902E−01


R6
5.4472E+01
1.2607E−03
−5.9916E−02
−1.6210E−02
1.0731E−02
1.2057E−02
8.9380E−03
6.3636E−03


R7
0.0000E+00
−8.8723E−02
3.2210E−02
1.4470E−02
1.4401E−03
7.7278E−04
−9.4008E−04
−4.5181E−04


R8
0.0000E+00
−9.2219E−02
−1.8649E−02
9.6955E−04
1.1933E−03
3.2053E−03
2.9773E−03
4.2921E−04


R9
1.6834E+01
−6.1539E−02
2.5808E−03
1.7542E−03
−9.9991E−03
−1.7005E−03
8.3213E−04
8.8685E−04


R10
−3.0678E+00
−7.4751E−02
3.3659E−02
1.4796E−03
4.2216E−04
−4.3315E−04
−1.5101E−04
2.2776E−05


R11
0.0000E+00
2.7764E−03
4.9448E−03
7.6319E−05
−6.4755E−05
−1.2592E−06
4.8810E−07
1.3221E−08


R12
−1.2637E+01
−3.6666E−02
7.1847E−03
−1.3454E−03
9.7793E−05
2.2532E−06
−1.3537E−07
−1.9250E−08









The values in the embodiments 1 to 3 and the corresponding values of the parameters specified in the condition expressions (1) to (8) are listed in following table 7.
As shown in table 7, the embodiment 1 meets the condition expression (1) to (8).
FIG. 3 is the diagram of the spherical aberration (axial chromatic aberration) of the camera lens LA in the embodiment 1; FIG. 4 is the diagram of the magnification chromatic aberration; FIG. 5 is the diagram of the image side curving and distortion aberration; In addition, the image side curving S in FIG. 5 is the image side curving relative to sagittal plane; T is the image side curving relative to the tangent plane. It is same also in embodiment 2 and 3. In embodiment 1, the camera lens LA with 2ω=83.9°, TTL/IH=1.422, Fno=2.05 and ultra-thin, high-luminous flux and wide-angle lenses as shown in FIGS. 3 to 5 is easy to understand that it has excellent optical properties.
Embodiment 2
FIG. 6 is the structural diagram of the camera lens LA in the embodiment 2; The curvature radius R of the object side and image side of the first lens L1 to sixth lens L6, center thickness of the lenses and the distance d between the lenses, refractive power nd and Abbe number v of the camera lens LA in the embodiment 2 are shown in table 3. The cone constant k and aspherical coefficients are shown in table 4.











TABLE 3






R
d
nd
vd






















R1
1.92937
d1 =
0.571
nd1
1.5441
v1
56.12


R2
−16.04613
d2 =
0.075






S1
∞
d3 =
−0.020






R3
3.44052
d4 =
0.220
nd2
1.6422
v2
22.41


R4
1.72032
d5 =
0.259






R5
28.59900
d6 =
0.221
nd3
1.6422
v3
22.41


R6
10.20990
d7 =
0.055






R7
5.84636
d8 =
0.466
nd4
1.5441
v4
56.12


R8
73.95723
d9 =
0.441






R9
−6.70148
d10 =
0.551
nd5
1.5441
v5
56.12


R10
−1.08873
d11 =
0.429






R11
−2.94315
d12 =
0.344
nd6
1.5441
v6
56.12


R12
1.79503
d13 =
0.520






R13
∞
d14 =
0.210
nd7
1.5168
v6
64.17


R14
∞
d15 =
0.298


















TABLE 4








Cone Constant
Aspherical Coeffecient
















k
A4
A6
A8
A10
A12
A14
A16


















R1
−8.3891E−01
6.6024E−04
4.6405E−03
−8.9822E−03
3.0454E−04
4.2769E−03
5.2521E−03
−1.2476E−02


R2
0.0000E+00
3.6167E−02
−1.5936E−02
−4.2482E−03
−2.1406E−03
−1.0377E−02
−5.9997E−02
4.8950E−02


R3
−1.5729E+01
−5.6059E−03
2.9056E−02
1.0013E−02
−2.7439E−02
−3.5585E−02
−6.4169E−02
9.4591E−02


R4
−4.3991E+00
−1.9461E−02
1.2210E−02
3.7679E−02
−4.7716E−02
−8.4170E−02
−4.8552E−02
1.9674E−01


R5
1.7584E+02
1.7091E−03
−1.0168E−01
−4.7142E−02
1.5618E−03
−2.5137E−02
−7.4424E−02
2.7064E−01


R6
5.3137E+01
1.3172E−03
−6.0752E−02
−1.6092E−02
1.1769E−02
1.3126E−02
9.4334E−03
5.9051E−03


R7
0.0000E+00
−8.9416E−02
3.1820E−02
1.3996E−02
6.9627E−04
1.7806E−04
−1.0612E−03
−1.4828E−04


R8
0.0000E+00
−9.0850E−02
−1.8199E−02
9.1377E−04
1.0705E−03
3.1196E−03
2.9401E−03
4.2003E−04


R9
1.7827E+01
−6.6702E−02
3.2192E−03
1.6088E−03
−1.0061E−02
−1.7276E−03
8.2262E−04
8.9045E−04


R10
−2.9964E+00
−7.5813E−02
3.3378E−02
1.4008E−03
4.1000E−04
−4.3674E−04
−1.5297E−04
2.1977E−05


R11
0.0000E+00
2.6978E−03
4.9309E−03
7.4527E−05
−6.5039E−05
−1.2582E−06
4.9632E−07
1.5915E−08


R12
−1.2325E+01
−3.6737E−02
7.1804E−03
−1.3454E−03
9.7837E−05
2.2644E−06
−1.3323E−07
−1.8891E−08









As shown in table 7, the embodiment 2 meets the condition expressions (1)-(8).
FIG. 7 is the diagram of the spherical aberration (axial chromatic aberration) of the camera lens LA in the embodiment 2; FIG. 8 is the diagram of the magnification chromatic aberration; FIG. 9 is the diagram of the image side curving and distortion aberration; As shown in FIGS. 7-9, in the embodiment 2, the camera lens LA, with full image angle 2ω=83.4°, TTL/IH=1.423, Fno=2.05, ultra-thin, high-luminous flux wide-angle lenses, is easy to understand that it has excellent optical properties.
Embodiment 3
FIG. 10 is the structural diagram of the camera lens LA in the embodiment 3; The curvature radius R of the object side and image side of the first lens L1 to sixth lens L6, center thickness of the lenses and the distance d between the lenses, refractive power nd and Abbe number v of the camera lens LA in the embodiment 3 are shown in table 5. The cone constant k and aspherical coefficient are shown in table 6.











TABLE 5






R
d
nd
vd






















R1
2.02102
d1 =
0.555
nd1
1.5441
v1
56.12


R2
−17.11059
d2 =
0.075






S1
∞
d3 =
−0.020






R3
2.95304
d4 =
0.217
nd2
1.6422
v2
22.41


R4
1.64342
d5 =
0.263






R5
27.56111
d6 =
0.222
nd3
1.6422
v3
22.41


R6
10.72823
d7 =
0.057






R7
5.92768
d8 =
0.464
nd4
1.5441
v4
56.12


R8
70.78538
d9 =
0.439






R9
−6.91410
d10 =
0.556
nd5
1.5441
v5
56.12


R10
−1.08764
d11 =
0.453






R11
−2.94590
d12 =
0.329
nd6
1.5441
v6
56.12


R12
1.79846
d13 =
0.520






R13
∞
d14 =
0.210
nd7
1.5168
v6
64.17


R14
∞
d15 =
0.277


















TABLE 6








Cone Constant
Aspherical Coeffecient
















k
A4
A6
A8
A10
A12
A14
A16


















R1
−8.5915E−01
4.8836E−04
4.4175E−03
−9.9818E−03
−1.4481E−03
2.7162E−03
5.2823E−03
−1.0259E−02


R2
0.0000E+00
2.9285E−02
−1.7790E−02
−4.1745E−03
−1.1523E−04
−6.2139E−03
−5.6190E−02
4.4117E−02


R3
−1.5308E+01
−6.1390E−03
2.7297E−02
8.2379E−03
−2.8709E−02
−3.5294E−02
−6.0228E−02
1.0591E−01


R4
−4.4960E+00
−2.1071E−02
1.0178E−02
3.6121E−02
−4.8696E−02
−8.3993E−02
−4.6594E−02
2.0146E−01


R5
8.2109E+01
1.4955E−03
−1.0112E−01
−4.5480E−02
3.1822E−03
−2.4910E−02
−7.6089E−02
2.6643E−01


R6
5.5628E+01
2.0009E−03
−5.9979E−02
−1.6231E−02
1.0773E−02
1.2118E−02
9.1342E−03
6.6540E−03


R7
0.0000E+00
−8.9844E−02
3.1474E−02
1.4097E−02
1.2617E−03
7.7182E−04
−9.2729E−04
−6.3490E−04


R8
0.0000E+00
−9.1044E−02
−1.8146E−02
1.0053E−03
1.1029E−03
3.1150E−03
2.9014E−03
3.7344E−04


R9
1.7699E+01
−6.6353E−02
3.3667E−03
1.5869E−03
−1.0124E−02
−1.7881E−03
7.8831E−04
8.7477E−04


R10
−2.9920E+00
−7.5761E−02
3.3415E−02
1.4223E−03
4.2110E−04
−4.3203E−04
−1.5213E−04
2.1376E−05


R11
0.0000E+00
2.7135E−03
4.9306E−03
7.4250E−05
−6.5026E−05
−1.2626E−06
4.9558E−07
1.5446E−08


R12
−1.2155E+01
−3.6764E−02
7.1779E−03
−1.3452E−03
9.7932E−05
2.2779E−06
−1.3235E−07
−1.8919E−08









As shown in table 7, the embodiment 3 meets the condition expressions (1) to (8).
FIG. 11 is the diagram of the spherical aberration (axial chromatic aberration) of the camera lens LA in the embodiment 3; FIG. 12 is the diagram of the magnification chromatic aberration; FIG. 13 is the diagram of the image side curving and distortion aberration; In embodiment 3, the camera lens LA2 with ω=84.4°, TTL/IH=1.416, Fno=2.05 ultra-thin, high-luminous flux wide-angle lenses, as shown in FIGS. 11 to 13, is easy to understand that it has excellent optical properties.
The values of the embodiments and the corresponding values of the parameters specified in the condition expressions (1) to (8) are listed in table 7. In addition, the units in table are 2ω (°), F (mm), F1 (mm), F2 (mm), F3 (mm), F4 (mm), F5 (mm), F6 (mm), TTL (mm), LB (mm), IH (mm).












TABLE 7







Embodi-
Embodi-
Embodi-




ment 1
ment 2
ment 3
Condition




















f1/f
0.96
0.89
0.95
1


f3/f
−5.19
−6.90
−7.80
2


(R3 + R4)/(R3 − R4)
3.90
3.00
3.51
3


d11/f
0.13
0.12
0.13
4


f2/f
−1.90
−1.57
−1.75
5


f4/f
3.27
3.23
3.36
6


(R1 + R2)/(R1 − R2)
−0.81
−0.79
−0.79
7


(R5 + R6)/(R5 − R6)
1.56
2.11
2.27
8


Fno
2.05
2.05
2.05


2ω
83.9
83.4
84.4


TTL/IH
1.422
1.423
1.416


f
3.565
3.602
3.526


f1
3.421
3.201
3.356


f2
−6.789
−5.640
−6.171


f3
−18.514
−24.842
−27.494


f4
11.663
11.639
11.860


f5
2.299
2.309
2.295


f6
−1.981
−1.998
−2.003


TTL
4.637
4.640
4.617


LB
0.999
1.028
1.007


IH
3.260
3.260
3.260









It is to be understood, however, that even though numerous characteristics and advantages of the present embodiments have been set forth in the foregoing description, together with details of the structures and functions of the embodiments, the disclosure is illustrative only, and changes may be made in detail, especially in matters of shape, size, and arrangement of parts within the principles of the invention to the full extent indicated by the broad general meaning of the terms in which the appended claims are expressed.

## Claims

1. A camera lens, comprising, from the object side to the image side:
a first lens with positive refractive power;
a second lens with negative refractive power;
a third lens with negative refractive power;
a fourth lens with positive refractive power;
a fifth lens with positive refractive power;
a sixth lens with negative refractive power, wherein
the camera lens satisfies the following specific conditions:


0.85≦f1/f≦1.10;



−10.00≦f3/f≦−4.50;



2.50≦(R3+R4)/(R3−R4)≦4.00;



0.08≦d11/f≦0.15;



where, f is the overall focal distance of the camera lens; f1 is the focal distance of the first lens; f3 is the focal distance of the third lens; R3 is the object side curvature radius of the second lens; R4 is the image side curvature radius of the second lens; d11 is the axial distance between the image side of the fifth lens and the object side of the sixth lens.

2. The camera lens according to claim 1 further satisfying the following specific condition:


−2.50≦f2/f≦−1.00


where, f is the overall focal distance of the camera lens; f2 is the focal distance of second lens.

3. The camera lens according to claim 1 further satisfying the following specific condition:


2.50≦f4/f≦6.00


where, f is the overall focal distance of the camera lens; f4 is the focal distance of the fourth lens.

4. The camera lens according to claim 1 further satisfying the following specific conditions:


−1.50≦(R1+R2)/(R1−R2)≦−0.50


wherein, R1 is the object side curvature radius of the first lens; R2 is the image side curvature radius of the first lens.

5. The camera lens according to claim 1 further satisfying the following specific conditions:


1.00≦(R5+R6)/(R5−R6)≦5.00


wherein, R5 is the object side curvature radius of the third lens; R6 is the image side curvature radius of the third lens.