Super wide-angle lens

1. A super wide-angle lens comprising, in order from an object side thereof:

a first lens with a negative refractive power, being a meniscus lens comprising a convex surface facing the object side;

a second lens with a negative refractive power;

a third lens with a positive refractive power; and

a fourth lens with a positive refractive power,

wherein each of the second lens and the fourth lens comprises at least one rotationally-asymmetric surface,

wherein the at least one rotationally-asymmetric surface of the second lens changes an aspect ratio in a horizontal direction and a vertical direction,

wherein the at least one rotationally-asymmetric surface of the fourth lens corrects a difference between shifts of focusing positions in the horizontal direction and the vertical direction which are caused on the at least one rotationally-asymmetric surface of the second lens, and

wherein the super wide-angle lens satisfies the following expressions:

0.5≦| f 2 x/f 4 x|≦ 2,

0.5≦| f 2 y/f 4 y|≦ 2

where f2 x is a paraxial focal length of the second lens in a XZ section,

f2 y is a paraxial focal length of the second lens in a YZ section,

f4 x is a paraxial focal length of the fourth lens in the XZ section, and

f4 y is a paraxial focal length of the fourth lens in the YZ section.

2. The super wide-angle lens of claim 1 ,

wherein the rotationally-asymmetric surface is an anamorphic surface in a shape defined by the following expression with a local Cartesian coordinate system (x, y, z) whose origin is on a top of the rotationally-asymmetric surface:

z =( CX·x 2 +CY·y 2 )/[1+√{1−(1+ KX )· CX 2 ·x 2 −(1+ KY )· CY 2 ·y 2 }]+AR ·[(1− AP )· x 2 +(1+ AP )· y 2 ] 2 +BR ·[(1− BP )· x 2 +(1+ BP )· y 2 ] 3 +CR ·[(1· CP )· x 2 +(1+ CP )· y 2 ] 4 +DR ·[(1− DP )· x 2 +(1+ DP )· y 2 ] 5 ,

where z is a displacement amount along a z-axis at a position of coordinates (x, y), the displacement amount being measured from the top of the rotationally-asymmetric surface,

each of CX and CY is a curvature at the top surface in a xz section and a yz section (=1/curvature radius),

KX and KY are conic constants for the xz section and the yz section, respectively,

AR, BR, CR, and DR are rotationally symmetric coefficients of the 4th order, 6th order, 8th order, and 10th order deformations from a conic, respectively and

AP, BP, CP, and DP are rotationally-asymmetric coefficients of 4th order, 6th order, 8th order, and 10th order deformations from a conic, respectively.

3. The super wide-angle lens of claim 1 ,

wherein the rotationally-asymmetric surface is a free-form surface in a shape defined by the following expression with a local Cartesian coordinate system (x, y, z) whose origin is on a top of the rotationally-asymmetric surface:

z=c·h 2 /[1+√{1−(1+ K )· c 2 ·h 2 }]+mΣnΣ[C ( m,n )· x m ·y n ],

where z is a displacement amount along a z-axis at a height h, the displacement amount being measured from a top of the surface,

h is a height in a direction perpendicular to the z-axis where h 2 =x 2 +y 2 ,

c is a curvature at the top of the surface, represented by 1/curvature radius,

K is a conic constant, and

C(m, n) is a free-form-surface coefficient where m, n=0, 1, 2 . . . .

4. The super wide-angle lens of claim 1 ,

wherein the super wide-angle lens satisfies the following expression:

ν d 3<50,

where νd3 is an Abbe number of the third lens.

5. The super wide-angle lens of claim 1 ,

wherein the super wide-angle lens satisfies the following expression:

ω X> 150 deg,

where ωX is a maximum of a total angle of view in a longitudinal direction.

6. The super wide-angle lens of claim 1 , further comprising:

an aperture stop arranged between the third lens and the fourth lens.